JP4124986B2 - Micro structure, micro mechanical quantity sensor, micro actuator, micro optical deflector, and optical scanning display - Google Patents

Description

[0001]
BACKGROUND OF THE INVENTION
The present invention relates to the field of micromachines or microstructures. More specifically, the present invention relates to a micro mechanical quantity sensor, a micro actuator, a micro optical deflector, and the like having a member that swings around an axis.
[0002]
[Prior art]
It is well known that, when trying to reduce the size of a mechanical element, the proportion of surface force becomes larger than the body force, and the influence of friction becomes larger than that of a normal size machine. For this reason, in designing a micromachine, it is common to consider to minimize the sliding part and the rotating part.
[0003]
A conventional example of an optical deflector having a member that swings around an axis will be described. FIG. 23 is a perspective view of an optical deflector disclosed in US Pat. No. 4,317,611. FIG. 24 is an exploded view of the optical deflector for explaining the internal structure. 25 and 26 show sectional views of the silicon thin plate 1020 taken along the cutting lines 1003 and 1006 in FIG. 23, respectively.
[0004]
In the optical deflector, a recess 1012 is formed in the substrate 1010 made of an insulating material. A pair of drive electrodes 1014 and 1016 and a mirror support portion 1032 are disposed on the bottom of the recess portion 1012. The silicon thin plate 1020 is integrally formed with torsion bars 1022 and 1024 and a mirror 1030. The mirror 1030 has a surface coated with a material having high light reflectivity, and is supported by torsion bars 1022 and 1024 so as to freely swing. The silicon thin plate 1020 is disposed on the substrate 1010 so as to keep a predetermined distance from the drive electrodes 1014 and 1016.
[0005]
Here, the silicon thin plate 1020 is electrically grounded. Therefore, by alternately applying a voltage to the drive electrodes 1014 and 1016, an electrostatic attractive force is applied to the mirror 1030, and the mirror 1030 can be swung around the major axes of the torsion bars 1022 and 1024.
[0006]
The cross-sectional shape of the torsion bars 1022, 1024 is a trapezoid as shown in FIG. However, the micro structure having a torsion bar having such a cross-sectional shape has a problem that the torsion bar is easy to bend, so that external vibrations are picked up and the shaft of the torsion bar is shaken, so that it cannot be driven accurately. was there.
[0007]
Therefore, when such an optical deflector is applied to an optical scanning display, there are problems that an image is blurred or a spot shape is changed due to external vibration. This becomes a bigger problem when the optical scanning display is made easy to carry.
[0008]
In order to make the torsion bar difficult to bend, the following structure has been proposed. FIG. 27 is a gimbal for a hard disk head disclosed in 10th International Conference on Solid-State Sensors and Actuators (Transducers '99) pp. 1002-1005. This gimbal is attached to the tip of a hard disk head suspension and is used to elastically allow the magnetic head to move between the roll and the pitch. The gimbal 2020 has a support frame 2031 that is rotatably supported by roll torsion bars 2022 and 2024 on the inner side. In addition, a head support 2030 that is rotatably supported by pitch torsion bars 2026 and 2028 is formed inside the support frame 2031. The torsion axes of the roll torsion bars 2022 and 2024 and the pitch torsion bars 2026 and 2028 (see the orthogonal chain lines in FIG. 27) are orthogonal to each other, and are responsible for the roll and pitch movement of the head support 2030, respectively. Yes.
[0009]
FIG. 28 is a cross-sectional view taken along the cutting line 2006 in FIG. As shown in FIG. 28, the torsion bar 2022 has a T-shaped cross section, and the gimbal 2020 has a rib structure.
[0010]
A manufacturing process of the present gimbal will be described with reference to FIGS. First, vertical etching is performed on the silicon wafer 2091 for molding using an etching method such as ICP-RIE (inductively coupled plasma-reactive ion etching) (a). This mold-taking silicon wafer 2091 can be reused. Next, a sacrificial layer 2092 made of a silicon oxide film and phosphorylated glass is formed on the mold-taking silicon wafer 2091 (b). Subsequently, a polysilicon layer 2093 serving as a structure is formed (c). Then, the polysilicon layer 2093 is patterned (d). Finally, the sacrificial layer 2092 is removed, and a polysilicon layer 2093 is bonded to the patterned pad 2095 with an epoxy resin 2094 (e).
[0011]
The torsion bar having a T-shaped cross section thus produced has a small cross-sectional secondary moment I, although the cross-sectional secondary pole moment J is smaller than that of a torsion bar having a cross-sectional shape such as a circular cross section or a rectangular cross section. There is a feature that is large. Therefore, it is possible to provide a torsion bar that is not easily bent while being relatively easily twisted. That is, it is possible to provide a torsion bar having high rigidity in a direction perpendicular to the torsion axis while ensuring sufficient compliance in the torsion direction.
[0012]
Further, since a torsion bar having a short length for obtaining a required compliance and an allowable torsion angle can be provided, there is an advantage that the size can be further reduced.
[0013]
Thus, by using the torsion bar having the T-shaped cross section, it is possible to provide a micro gimbal having sufficient compliance in the roll and pitch directions and sufficient rigidity in the other directions and capable of further miniaturization.
[0014]
[Problems to be solved by the invention]
However, this microstructure has the following problems.
1. A torsion bar having a T-shaped cross section is fragile due to stress concentration at the portion 2050 in FIG. 28 when twisted.
2. In the torsion bar having a T-shaped cross section, the center of torsion and the center of the center of gravity axis do not coincide. Therefore, an excitation force in a direction perpendicular to the torsion axis is generated during the swinging. Therefore, an unnecessary movement occurs during driving.
3. Since polysilicon has a larger internal loss than single crystal silicon, the mechanical Q value is lowered. Therefore, the vibration amplitude cannot be increased when driving using mechanical resonance. In addition, energy efficiency is low due to large loss.
[0015]
An object of the present invention is a micromachine or a micro structure that can be applied to a micro mechanical quantity sensor, a micro actuator, a micro optical deflector, etc. having a member that swings around an axis, in which such problems are solved.TheIt is to provide.
[0016]
[Means for Solving the Problems]
In order to solve the above problems, a microstructure of the present invention includes a substrate and a flat plate-like rocking body, and the rocking body is elastic to the substrate by a torsion bar.TorsionaxisThe centerThe substrate, the rocking body and the torsion bar are integrally formed of a single crystal material, and the torsion bar isA groove extending in parallel with the torsion axis is provided on each of an upper surface that is the same surface side as the surface side of the rocking body and a lower surface that is the same surface side as the back surface side thereof, and the width of the groove Wg And the distance between the upper surface and the lower surface t And Wg <t / tan54.7 Satisfy the relationship of °, andSaidTorsionCross section perpendicular to the axisofX shapeHaving a cross-sectional shape ofIt is characterized by that. The cross-sectional shape of the torsion spring perpendicular to the long axis (also referred to as the torsion spring cross-sectional shape or transverse cross-sectional shape in this specification) is the plane of the flat rocking body (in the micro optical deflector, this is the reflective surface, etc. In this case, it is possible to effectively realize a structure that is not easily bent in a direction perpendicular to or parallel to the plane of the oscillator.
[0017]
Based on this basic configuration, the following more specific forms are possible.
In the above basic configuration, the torsion spring's torsional central axis can be easily passed through the vicinity of the center of gravity of the flat plate-like rocking body. By adopting a configuration in which the torsion spring twist axis passes through the vicinity of the center of gravity of the oscillating body, the oscillating body can be stably torsionally vibrated. If the torsion spring's torsion shaft center does not match the center of gravity of the rocking body, this discrepancy is caused by the torsional vibration of the rocking body. Vibration and displacement are likely to occur. Therefore, unnecessary vibration of the micro structure such as the micro optical deflector can be reduced by adopting a configuration in which the axis of torsion passes through the vicinity of the center of gravity of the oscillator.
[0018]
The cross-sectional shape of the surface perpendicular to the long axis of the torsion spring can be easily made symmetrical with respect to the surface including the torsional central axis. The torsion spring has a cross-sectional shape that is inclined with respect to the plane of the oscillating body, and is further symmetric so that it can be easily twisted about the axis of the torsion, and further in a direction perpendicular to the torsion axis. It can be set as the structure which is hard to bend.
[0019]
The torsion spring is preferably made of a single crystal material such as silicon single crystal. In this way, it is possible to realize a rocking mechanism that can reduce internal loss and has high energy efficiency. Further, by using a single crystal material as a material, a mechanical high Q value structure can be realized. As the single crystal material, it is preferable to use single crystal silicon which is easily available and has excellent mechanical properties (that is, relatively light weight but excellent physical strength, resistance and life). By using a (100) silicon single crystal substrate, the inclined surface of the torsion spring can be easily made to be the (111) plane of silicon single crystal.
[0020]
Further, the single crystal material is a (100) silicon single crystal substrate, the torsion spring is formed by anisotropic etching, and the inclined surface with respect to the (100) substrate surface defining the outer surface is the (111) plane. Can be. At this time, the surface with respect to the (100) substrate surface that defines the outer surface of the base portion of the torsion spring connected to the substrate or the oscillating body can also be the (111) surface. Since the (111) plane is formed with high precision and smoothness, the produced torsion spring is difficult to break. Furthermore, if the surface of the base portion of the torsion spring is also a (111) slope, the stress concentration on the surface can be relaxed, and the reliability of the torsion spring can be improved.
[0021]
Typically, the substrate, the oscillator, and the torsion spring can be integrally formed by etching or the like from a single crystal material substrate such as a common silicon single crystal or crystal.
[0023]
Corners (such as steep wedges) of the torsion spring may be lightly rounded by isotropic etching to relieve stress concentration there.
[0024]
The cross-sectional shapes of two or more sets of torsion springs that support the rocking body may be different from each other with respect to the torsion springs that face each other with the rocking body interposed therebetween. As a result, it is possible to make the structure more difficult to bend in the direction perpendicular to the torsion axis while maintaining sufficient torsional compliance. In other words, in this structure, the directions in which the torsion springs facing each other across the rocking body are easy to bend are different. Therefore, the vibration or displacement of the rocking body in this direction which is not necessary in the micro structure such as the micro optical deflector. Can be reduced.
[0025]
Further, the cross-sectional shape of the torsion springs facing each other with the rocking body interposed therebetween is changed to a surface including the torsional central axis of the opposing torsion spring (this surface typically includes the torsional central axis of the opposing torsion spring. They may be arranged symmetrically with respect to each other with respect to a plane parallel to the plane of the oscillating plate. As a result, the directions in which the torsion springs are easily bent can be crossed symmetrically. Therefore, it is possible to effectively make the structure difficult to bend in the direction perpendicular to the axis of torsion, and this is a preferable form in which the opposing torsion springs have different shapes.
[0026]
As a form of the micro structure, there is one rocking body, and the rocking body rocks elastically about the straight line with respect to the substrate by one or a pair of torsion springs extending along the straight line. It can take the form of being supported freely. The form of the pair of torsion springs is described in the embodiments described later. However, when the rocking body is sufficiently lightweight and can be supported freely by one torsion spring without any trouble, such a form is also used according to the application. it can.
[0027]
As another form of the microstructure, there are a plurality of the oscillating bodies, the plurality of oscillating bodies are arranged in a nesting manner, and each oscillating body has a pair of torsion springs extending along each straight line. It is also possible to adopt a form in which the oscillating body or the substrate is supported so as to freely oscillate about the straight lines. An example in which two oscillating bodies are arranged in a nested manner is shown in FIG. If necessary, a configuration in which three or more oscillating bodies are arranged in a nested manner can be realized. The angle formed by the straight lines is typically 90 degrees (see the example of FIG. 27), but this may also be an angle other than 90 degrees if necessary.
[0028]
As another form of the microstructure, there are a plurality of the oscillating bodies, the plurality of oscillating bodies are arranged in series with a torsion spring interposed therebetween, and the outermost oscillating body has a torsion spring on the substrate. The form supported by interposing can also be taken. For example, a relatively small mass oscillating body is sandwiched between relatively large mass oscillating bodies via a torsion spring, and large mass oscillating bodies on both sides are connected to a substrate via a torsion spring, and these three torsion springs are connected. As a form extending along a straight line, in this form, a small mass oscillator is indirectly driven by driving a large mass oscillator. In any case, the microstructure of the present invention is characterized in that at least a part of the cross-sectional shape of the torsion spring is inclined with respect to the plane of the plate-like rocking body, and the form depends on the application. It can be various.
[0029]
Furthermore, a micro mechanical quantity sensor of the present invention for solving the above-mentioned problems is characterized by having the above-described microstructure and displacement detecting means for detecting the relative displacement between the substrate and the oscillator. As the displacement detection means, conventionally known ones can be used. For example, there is one that detects the relative displacement between the substrate and the rocking body by detecting the change in capacitance by the change in voltage. Specific examples thereof are disclosed in JP-A-8-145717, JP-A-2000-65664, JP-A-2000-292434, and the like.
[0030]
Furthermore, a microactuator of the present invention for solving the above-described problems is characterized by having the above-described microstructure and driving means for driving the rocking body relative to the substrate. The driving means includes a fixed core, a coil that circulates around the fixed core (formed of a soft magnetic material), and a movable core (soft magnetic or hard magnetic permanent magnet) joined to the oscillator. The driving principle is different between the two, and in the former, the magnetic pole of the soft magnetic material is not determined, and when the magnetic flux is generated in the fixed core, the magnetic flux is cut in the direction of increasing the cross-sectional area of the soft magnetic material that cuts the magnetic flux of the magnetic circuit. In the latter case, the magnetic pole of the hard magnetic material is fixed, and the magnetic force between the fixed core and the movable core is different or between the same magnetic poles. The magnetic actuator (attractive force or repulsive force) is the driving force), or uses an electrostatic attractive force.
[0031]
Furthermore, a micro optical deflector of the present invention for solving the above-described problems includes the above-described microstructure, driving means for driving the oscillator relative to the substrate, and light provided in the oscillator. It has a deflector. The driving means is as described above. The light deflector includes a light reflecting surface or a diffraction grating. In the latter case, one beam can be deflected as a plurality of beams (diffracted light).
[0032]
Furthermore, an optical scanning display of the present invention for solving the above-described problems includes a micro light deflector, a light source (such as a semiconductor laser) that can be modulated, modulation of the light source, and oscillation of the micro light deflector. It has the control means which controls operation | movement of a moving body, It is characterized by the above-mentioned.
[0035]
[Action]
The operation of the microstructure of the present invention will be described.
In the microstructure of the present invention, as described above, the cross-sectional shape of the torsion spring is inclined with respect to the plane of the oscillating body (in the micro optical deflector, a deflector such as a reflecting surface is provided here). Therefore, it is possible to effectively realize a structure that is not easily bent in a direction perpendicular to or parallel to the plane of the oscillator (the reflection surface of the micro light deflector). For example, in a micro light deflector, a functional element of an actuator (for example, in the case of an electrostatic drive type actuator) on a surface on which a reflecting surface of an oscillating body is not formed (that is, a surface opposite to a reflecting surface forming surface or a side surface of the oscillating body) Therefore, vibration and displacement due to unnecessary generated forces in the vertical and parallel directions are likely to occur with respect to the reflecting surface. Therefore, by forming the inclined portion in the cross-sectional shape of the torsion spring, the rigidity against the vertical and parallel bending can be increased with a simple structure, and the unnecessary vibration of the micro optical deflector can be reduced.
[0036]
DETAILED DESCRIPTION OF THE INVENTION
Hereinafter, in order to clarify the embodiment of the present invention, examples will be described with reference to the drawings.
[0037]
[Example 1]
FIG. 1 is a perspective view for explaining a micro optical deflector according to a first embodiment of the present invention. FIG. 2 is an exploded view of the micro optical deflector for explaining the internal structure. FIG. 3 is a cross-sectional view taken along the cutting line 109 in FIG. 2 for explaining the operation of the micro optical deflector of the present embodiment. FIG. 4 is a cross-sectional view for explaining the structure of the torsion spring, which is a feature of this embodiment, and shows a cross section of the silicon single crystal thin plate 120 taken along the cutting line 106 in FIG.
[0038]
In the micro optical deflector according to the first embodiment, the glass substrate 110 has a recess 112 formed therein. A pair of drive electrodes 114 and 116 and a triangular prism-shaped mirror support portion 132 are disposed on the bottom of the recess 112. The mirror support portion 132 may be omitted if possible. The torsion springs 128 and 129 and the mirror 130 are integrally formed on the silicon single crystal thin plate 120 by bulk micromachining technology. As shown in FIG. 4, the torsion springs 128 and 129, which are the features of the present embodiment, have a V-shaped cross section that is symmetric. This is a heptagon with one interior angle of 289.4 °, and has two cross-sectional shapes inclined with respect to the plane of the mirror 130.
[0039]
The mirror 130 is formed by coating a surface of a flat plate with a material having high light reflectivity, and is supported by V-shaped torsion springs 128 and 129 so as to freely swing around the major axis. The silicon single crystal thin plate 120 is disposed on the glass substrate 110 so that the mirror 130 keeps a predetermined distance from the drive electrodes 114 and 116 (FIG. 3). The lower surface of the mirror 130 along the long axis of the torsion springs 128 and 129 is in contact with the top line part of the mirror support part 132 as shown in FIG. 3, and the mirror 130 is rotated around the swing axis along the top line part. It can swing.
[0040]
The silicon single crystal thin plate 120 is electrically grounded. Therefore, by alternately applying a voltage to the drive electrodes 114 and 116, the mirror 130 can be swung around the swinging shaft by applying an electrostatic attractive force to the mirror 130. The driving force is not limited to electrostatic attraction, but magnetic force can also be used. In this case, an electromagnet is installed instead of the drive electrode, and a hard magnetic material magnet is fixed to the lower surface of the mirror 130.
[0041]
A method for manufacturing the optical deflector will be described in detail below with reference to FIGS. 6A to 6E show cross sections along the cutting line 106 in FIG. 1, and FIGS. 7A to 7E show cross sections along the cutting line 109 in FIG.
[0042]
First, processing of the silicon single crystal thin plate 120 will be described with reference to FIG.
[0043]
1. A mask layer 150 (for example, SiO 2) is formed on both sides of the silicon single crystal thin plate 120.₂Or silicon nitride produced by a low pressure chemical vapor deposition method). As the silicon single crystal thin plate 120, a (100) substrate is used. Then, the mask layer 150 is patterned by photolithography (a). In FIG. 6, the width W on the upper surface side and the lower surface side of the substrate 120, respectively._aOne opening and width W_bAre formed. Width W_bThe striped mask layer 150 between the two openings has a width W_aIt extends corresponding to the center line of the opening. Width W_aIs approximately set to the width of the uppermost opening of the V-shaped torsion springs 128, 129, and the width W_bThe width of the striped mask layer 150 between the two openings is substantially set to the width of the bottom of the V-shaped torsion springs 128 and 129.
[0044]
2. Etching is performed from both sides of the silicon single crystal thin plate 120 using an anisotropic etching solution which is an alkaline solution such as KOH. Since anisotropic etching of silicon proceeds fast on the (100) plane and proceeds slowly on the (111) plane, the etching first proceeds so that the opening becomes narrower as the digging progresses (b, c). At this time, the side surface of the etched portion is a smooth (111) surface.
[0045]
3. W_bIn the opening having a width of 2 mm, etching proceeds until the substrate 120 is penetrated._aIn the opening having the width of, etching stops before passing through the substrate 120, and the bottoms of the V-shaped torsion springs 128 and 129 are formed (d). As shown in FIG. 5, since the (111) plane has an angle of 54.7 degrees with respect to the (100) plane, the relationship between the width w of the opening and the depth d of the V groove is d = w / 2 ・ tan54.7 °. Accordingly, since the V-shaped torsion springs 128 and 129 are formed as described above, W_a<2t / tan54.7 °, W_bThe relationship of> 2t / tan54.7 ° is satisfied. Here, t is the thickness of the silicon single crystal thin plate 120.
[0046]
As described above, since the etching from the upper surface becomes the (111) plane before the bottom surface of the substrate 120 is reached and the etching stops, a V-shaped groove is formed. Etching from the lower surface proceeds until it penetrates the substrate 120 and stops at the mask layer 150.
[0047]
At this time, the mask layer 150 on the lower surface side is patterned so that other etching penetration portions around the mirror 130 are also formed. Further, since the (111) plane is formed with high precision and smoothness, the manufactured V-shaped torsion springs 128 and 129 are difficult to break. Further, by the anisotropic etching, the surfaces of the V-grooves at the bases of the torsion springs 128 and 129 (indicated by 128a and 129a in FIG. 2A) are also (111) slopes as shown in FIG. As a result, the concentration of stress can be relaxed, the reliability of the torsion spring can be improved, and the light deflection angle of the mirror can be increased.
[0048]
4). After the anisotropic etching, isotropic etching may be performed with gas or acid to round the corners of the sharp wedge portion of the V groove and the corner portion of the torsion spring. In this way, stress concentration on these portions can be alleviated.
[0049]
5. Next, the mask layer 150 is removed (e).
6). Finally, the mirror 130 is cleaned, and a light reflecting film is formed on the surface.
[0050]
Next, a method for processing the glass substrate 110 will be described with reference to FIG.
1. A mask layer 151 (resist or the like) is formed on both surfaces of the glass substrate 110 (a).
[0051]
2. The mask layer 151 is patterned (b). Patterning is performed so that the triangular pillar-shaped mirror support portion 132 and the recessed portion 112 are formed by etching.
3. Etching is performed so that the depth of the recess 112 becomes 25 μm (c). At this time, a triangular prism-shaped mirror support portion 132 is formed.
[0052]
4). The mask layer 151 is removed, and drive electrodes 114 and 116 having a predetermined pattern are formed in the recess 112 (d).
[0053]
5. The silicon single crystal thin plate 120 and the glass substrate 110 are bonded so as to form a micro optical deflector as shown in FIG. 1 (e).
[0054]
As described above, according to the manufacturing method of the present embodiment, the torsion springs 128 and 129 having V-shaped cross sections can be manufactured by performing anisotropic etching only once. As shown in FIG. 4, the torsion spring 128 (129) of the optical deflector according to the present embodiment having a V-shaped cross section is easily twisted and is not easily bent like the conventional torsion bar having a T-shaped cross section. It has a structure. Further, the cross-sectional shape of the torsion springs 128 and 129 has two intersecting portions that are inclined with respect to the plane (mirror 130) of the flat plate-like oscillating body, so that it bends in a direction perpendicular to and parallel to the plane of the oscillating body. It has a difficult structure. Furthermore, according to the present embodiment, by using single crystal silicon as a material for the torsion spring, it is possible to realize a microstructure having a mechanical Q value larger than that of polysilicon.
[0055]
Furthermore, according to the present embodiment, by using a single crystal material as the material of the torsion spring, it is more difficult to break, can be downsized, and has a large vibration amplitude and high energy efficiency when resonance driven. Can be realized. In addition, by using the manufacturing method of this embodiment, the microstructure of this embodiment can be manufactured relatively easily.
[0056]
A modification of the first embodiment will be described. FIG. 8A is a perspective view for explaining the micro optical deflector of the present modification. The torsion springs 628 and 629 have a V-shaped cross section or an inverted V-shaped cross section surrounded by the substrate surface and the (111) plane of silicon. The side surfaces of the mirror 630 and the frame body 620 on which the reflection surface is formed are shapes in which the (111) surface of silicon is exposed, but in FIG. 8, the side surfaces are drawn as side surfaces perpendicular to the reflection surface for simplicity. . The same applies to other drawings.
[0057]
Unlike the first embodiment, the micro optical deflector of this modification is characterized in that the cross-sectional shapes of the two sets of torsion springs 628 and 629 are different as shown in FIG. Thereby, it is possible to provide a structure that is easily twisted and is less likely to bend. Further, at the time of torsional resonance driving, the influence of an unnecessary motion mode such as flexural vibration generated due to the structure of one torsion pulling 628 or 629 or disturbance can be canceled by the structure of the other torsion pulling 629 or 628. , Driving stability can be improved.
[0058]
Specifically, as shown in FIG. 8B, the shape of the torsion springs 628 and 629 in the section AA ′ and the shape of the section BB ′ in the substrate surface (the torsional central axes of the torsion springs 628 and 629). And a plane parallel to the plane of the mirror 630). Further, the center of gravity of the mirror 630 coincides with the torsional rotation axes of the two sets of torsion springs 628 and 629, and the driving stability can be further improved.
[0059]
The micro optical deflector according to this modification is produced by processing a silicon substrate using crystal anisotropic etching, as in the first embodiment. The manufacturing process described with reference to FIG. 6 may be used, but the mask layer 150 on which the other torsion spring is formed is upside down from the pattern of FIG. In this manner, the torsion springs 628 and 629 in which the portions having the flat cross section are combined upside down can be easily manufactured by performing anisotropic etching only once.
[0060]
According to this modification, it is possible to realize a micro optical deflector that can be easily processed, and that the cross-sectional shapes of the two sets of torsion springs are different from each other, thereby canceling the influence of disturbances during driving caused by the respective torsion springs.
[0061]
[Example 2]
FIG. 9 is a perspective view for explaining the micro optical deflector according to the second embodiment of the present invention. FIG. 10 is an exploded view of the micro light deflector for explaining the internal structure. FIG. 11 shows a cross section of the silicon single crystal thin plate 120 taken along the cutting line 106 in FIG. 10 is the same as FIG. 3.
[0062]
Also in the micro optical deflector of the second embodiment, the glass substrate 110 has a recess 112 formed therein. A pair of drive electrodes 114 and 116 and a triangular prism-shaped mirror support portion 132 are disposed on the bottom of the recess 112. The silicon single crystal thin plate 120 is integrally formed with torsion springs 122 and 124 and a mirror 130 by bulk micromachining technology. As shown in FIG. 11, the torsion springs 122 and 124, which are the features of the present embodiment, have an X-shaped cross section. As is apparent from FIG. 11, this shape is a dodecagon whose four inner angles are larger than 180 degrees, and is a rotationally symmetric shape. Furthermore, the cross-sectional shape part which cross | intersected with respect to the plane of the mirror 130 is included.
[0063]
The mirror 130 is formed by coating a material having a high light reflectance on the surface of a flat plate, and is swingably supported around the major axis by X-shaped torsion springs 122 and 124. The silicon single crystal thin plate 120 is disposed on the glass substrate 110 so that the mirror 130 keeps a predetermined distance from the drive electrodes 114 and 116. The lower surface of the mirror 130 along the long axis of the torsion springs 122 and 124 is in contact with the top line part of the mirror support part 132, and the mirror 130 can swing around the swing axis along the top line part. Yes.
[0064]
The silicon single crystal thin plate 120 is electrically grounded. Therefore, by alternately applying a voltage to the drive electrodes 114 and 116, the mirror 130 can be swung around the swinging shaft by applying an electrostatic attractive force to the mirror 130.
[0065]
A method for manufacturing the optical deflector will be described in detail below with reference to FIGS. The process of FIG. 7 is also used in this embodiment. 13A to 13G represent cross sections along the cutting line 106 in FIG. 9, and FIGS. 7A to 7E represent cross sections along the cutting line 109 in FIG.
[0066]
The processing of the silicon single crystal thin plate 120 will be described with reference to FIG.
[0067]
1. A mask layer 150 (for example, SiO 2) is formed on both sides of the silicon single crystal thin plate 120.₂Or silicon nitride produced by a low pressure chemical vapor deposition method). As the silicon single crystal thin plate 120, a (100) substrate is used. Then, the mask layer 150 is patterned by photolithography (a). FIG. 12 shows a mask pattern used for this patterning. The mask pattern shown in FIG. 12 is formed along the outer shapes of the torsion springs 122 and 124 and the mirror 130._aAnd an opening 191 having a width of W is formed._bW along the longitudinal centerline of the torsion spring_gAn opening 190 having a width of 1 mm is formed.
[0068]
2. Etching is performed from both sides of the silicon single crystal thin plate 120 using an anisotropic etching solution which is an alkaline solution such as KOH. Since anisotropic etching of silicon proceeds fast on the (100) plane and proceeds slowly on the (111) plane, the etching first proceeds so that the opening becomes narrower as the digging progresses (b).
[0069]
3. In the opening 190 having a width of Wg, all the surfaces become the (111) surface before etching reaches the center of the substrate 120, and the etching stops, so that the V-shaped groove (as shown in FIG. dg and width Wg). In the opening 191 having a width of Wa, etching proceeds until the substrate 120 is penetrated (c). As shown in FIG. 5, since the (111) plane has an angle of 54.7 degrees with respect to the (100) plane, the relationship between the width w of the opening and the depth d of the V groove is d = w. /2·tan54.7°. Therefore, hereWg <t / tan54.7 ° Wa> t / tan54.7 °Meet the relationship. Here, t is the thickness of the silicon single crystal thin plate 120.
[0070]
4). After the holes from above and below the opening 191 penetrate, the etching proceeds to the side (d, e).
[0071]
5. The etching stops when the (111) plane is reached. At this time, the cross sections of the torsion springs 122 and 124 are X-shaped (f). As shown in FIG. 11, the depth of the V groove on the side of the X-shaped cross section is k_bAnd the width is t. At this time, since the (111) plane is formed with high accuracy and smoothness, the produced X-shaped torsion springs 122 and 124 are difficult to break. Further, by the anisotropic etching, the surfaces of the V-grooves at the bases of the torsion springs 122 and 124 (shown by 122a and 124a in FIG. 10A) are also formed as (111) slopes as shown in FIG. 10B. Therefore, the stress concentration here can be relaxed, the reliability of the torsion spring can be improved, and the light deflection angle of the mirror can be increased.
[0072]
6). After the anisotropic etching, isotropic etching may be performed with gas or acid to round the corners of the sharp wedge portion of the V groove and the corner portion of the torsion spring. In this way, stress concentration on these portions can be alleviated.
[0073]
7. Next, the mask layer 150 is removed (g).
8). Finally, the mirror 130 is cleaned, and a light reflecting film is formed on the surface.
[0074]
About the processing method of the glass substrate 110, it is the same as description of Example 1 described along FIG.
[0075]
As described above, according to the manufacturing method of this embodiment, the torsion springs 122 and 124 having an X-shaped cross section can be manufactured by performing anisotropic etching only once. As shown in FIG. 11, the torsion spring 122 (124) of the optical deflector according to the present embodiment having an X-shaped cross section has a large sectional secondary moment I for a small sectional secondary pole moment J. There are features. In addition, since the cross-sectional shape is rotationally symmetric, it is possible to realize a micro structure that does not generate an excitation force in a direction perpendicular to the torsion axis when swinging. Furthermore, since the cross-sectional shape of the torsion springs 122 and 124 has an intersecting portion inclined with respect to the plane (mirror 130) of the flat plate-like oscillating body, it is more difficult to bend in the direction perpendicular to and parallel to the plane of the oscillating body. It has a structure.
[0076]
Also in this embodiment, by using single crystal silicon as a material for the torsion spring, it is more difficult to break than polysilicon and can be downsized, and has a large vibration amplitude and high energy efficiency when driven by resonance. A microstructure with a large mechanical Q value can be realized.
[0077]
In addition, since it is difficult to vibrate in the direction perpendicular to the axis of the torsion spring when it swings, a highly accurate micro optical deflector can be realized, and since the mechanical Q value is high, the vibration amplitude is large when driven by resonance. An energy efficient micro optical deflector can be realized. Furthermore, by using the manufacturing method of the present embodiment, a torsion spring having an X-shaped cross section can be manufactured relatively easily.
[0078]
A modification of the second embodiment will be described. FIG. 14A is a perspective view for explaining the micro optical deflector of the present modification. The torsion springs 728 and 729 have a flat cross section surrounded by the substrate surface 720 and the (111) surface of silicon.
[0079]
Unlike the second embodiment, the micro optical deflector of the present modification is characterized in that the two sets of torsion springs 728 and 729 have different cross-sectional shapes. As a result, it is possible to provide a structure that is easy to twist and is less likely to bend. In addition, during torsional resonance drive, unnecessary motion modes such as flexural vibration caused by one torsion bar structure and the influence of disturbance can be canceled by the other torsion bar structure, and drive stability can be improved. .
[0080]
Specifically, as shown in FIG. 14B, the shape of the AA ′ cross section of the torsion bar 728 and the shape of the BB ′ cross section of the torsion bar 729 are also the substrate surface 720 (the surface of the mirror 730). More precisely, the figure is symmetrical with respect to a plane parallel to the plane of the mirror 730 including the torsional central axes of the torsion bars 728 and 729. Further, the center of gravity of the two sets of torsion bars 728 and 729 (also the center of gravity of the mirror 730) coincides with the torsional rotation axis, and the driving stability can be further improved.
[0081]
The micro optical deflector according to the present modification is produced by processing a silicon substrate using crystal anisotropic etching, as in the second embodiment. FIG. 15 is a cross-sectional view showing a manufacturing process.
[0082]
First, mask layers 731 and 732 made of silicon nitride are formed on both surfaces of a single crystal silicon substrate 720 having a plane orientation (100) by low pressure chemical vapor deposition (see FIG. 15A). Next, photolithography and CF₄The mask layers 731 and 732 are patterned by dry etching using gas (see FIG. 15B). Here, the mask layer is left on the upper and lower surfaces of the substrate 720 by the width of the torsion bar, and the remaining mask layer portions are shifted to the left and right according to the inclination of the torsion bar. Next, crystal anisotropic etching of silicon 720 is performed using a 30% aqueous potassium hydroxide solution heated to 100 ° C. (see FIG. 15C). Further, by continuing this etching, the substrate 720 is penetrated (see FIG. 15D). The etching direction at this time is as shown in the figure. Further, by continuing the above etching, a plate spring-like torsion bar 728 or 729 whose side surface is made of a Si (111) surface is formed (see FIG. 15E). The other torsion bar 729 or 728 on the opposite side across the mirror 730 is also formed, but in this part, the mask layer is patterned in an upside down manner with respect to FIG. 15 and anisotropic etching is performed. .
[0083]
Here, the mask layer may be removed. Further, a reflective film may be formed on the surface of the reflective surface. As described above, according to the manufacturing method of this modification, a torsion spring combining the torsion bars 728 and 729 having a flat cross section can be easily manufactured by performing anisotropic etching only once.
[0084]
According to this modification, the following micro optical deflector can be provided. Here, the two sets of torsion springs each have a simple structure of one leaf spring, the process is easy, and the two sets of torsion springs have different cross-sectional shapes, so that a structure that is easy to twist and more difficult to bend is obtained. In addition, it is possible to cancel the influence of disturbances during driving caused by the respective torsion springs. In addition, the center of gravity of the two sets of torsion bars and the torsional rotation axis can be easily matched, the drive can be stabilized easily, and the torsion bar has no stress concentration part and has a structure that is difficult to break. .
[0085]
[Example 3]
FIG. 16 is a perspective view for explaining the micro optical deflector according to the third embodiment of the present invention. FIG. 17 is an exploded view of the micro light deflector for explaining the internal structure. FIG. 18 is a cross-sectional view showing a cross section of the silicon single crystal thin plate 120 taken along the cutting line 106 in FIG. 17 is the same as FIG. 3.
[0086]
Also in the micro optical deflector of the third embodiment, the glass substrate 110 has a recess 112 formed therein. A pair of drive electrodes 114 and 116 and a triangular prism-shaped mirror support portion 132 are disposed on the bottom of the recess 112. The torsion springs 128 and 129 and the mirror 130 are integrally formed on the silicon single crystal thin plate 120 by bulk micromachining technology. The torsion springs 128 and 129, which are the features of the present embodiment, are arranged in a pair of flat torsion bars 122, 123; 124, 125 as shown in FIG. Is made up of.
[0087]
The mirror 130 is formed by coating a surface of a flat plate with a material having a high light reflectivity, and is supported by torsion springs 128 and 129 so as to freely swing. The silicon single crystal thin plate 120 is disposed on the glass substrate 110 so that the mirror 130 keeps a predetermined distance from the drive electrodes 114 and 116. The lower surface of the mirror 130 along the torsion axis of the torsion springs 128 and 129 is in contact with the top line part of the mirror support part 132, and the mirror 130 can swing around the swing axis along the top line part. Yes.
[0088]
The silicon single crystal thin plate 120 is electrically grounded. Therefore, by alternately applying a voltage to the drive electrodes 114 and 116, the mirror 130 can be swung around the swinging shaft by applying an electrostatic attractive force to the mirror 130. These configurations are the same as those in the first and second embodiments.
[0089]
A method for manufacturing the optical deflector of this example will be described in detail below with reference to FIGS. The process of FIG. 7 is also used in this embodiment. 19A to 19E represent cross sections along the cutting line 106 in FIG. 16, and FIGS. 7A to 7E represent cross sections along the cutting line 109 in FIG.
[0090]
The processing of the silicon single crystal thin plate 120 will be described with reference to FIG.
1. A mask layer 150 (for example, SiO 2) is formed on both sides of the silicon single crystal thin plate 120.₂Or silicon nitride produced by a low pressure chemical vapor deposition method). As the silicon single crystal thin plate 120, a (100) substrate is used. Then, the mask layer 150 is patterned by photolithography (a). This mask pattern has a width W on the upper surface side and the lower surface side of the substrate 120 at the portions of the torsion springs 128 and 129, respectively._aAnd width W_bStripe-shaped openings are formed. Width W_bA pair of stripe openings are formed with a stripe mask layer 150 in between and a width W_aOne stripe-shaped opening is formed at the upper surface portion corresponding to the stripe-shaped mask layer. Width W_aIs set to the distance at the top of the two torsion bars 122, 123; 124, 125, and the width W_bThe width of the striped mask layer 150 between the two openings is set to the distance between the bottoms of the two torsion bars 122, 123; 124, 125. In this mask pattern, an opening having an appropriate width is also formed on the upper surface side of the substrate 120 along the outer shape of the mirror 130.
[0091]
2. Etching is performed from both sides of the silicon single crystal thin plate 120 using an anisotropic etching solution which is an alkaline solution such as KOH. Since anisotropic etching of silicon proceeds fast on the (100) plane and proceeds slowly on the (111) plane, the etching first proceeds so that the opening becomes narrower as the digging progresses (b, c).
[0092]
3. Etching proceeds until the substrate 120 penetrates from both sides, and stops at the mask layer 150 (d). As shown in FIG. 5, since the (111) plane of silicon has an angle of 54.7 degrees with respect to the (100) plane, the relationship between the width w of the opening and the depth d of the V groove is d = w / 2 · tan54.7 °. Therefore, in order to penetrate the substrate 120, W_a, W_bIt is necessary to satisfy the relationship> 2t / tan54.7 °. Here, t is the thickness of the silicon single crystal thin plate 120.
[0093]
At this time, since the (111) plane is formed with high precision and smoothness, the manufactured torsion springs 128 and 129 having a reverse cross-sectional shape are difficult to break. Further, by the anisotropic etching, the surfaces of the V-grooves at the base portions of the torsion springs 128 and 129 (indicated by 128a and 129a in FIG. 17A) are also shown in FIG. 17B (the cutting line in FIG. 17A). As shown in 190 (cross-sectional view of the silicon single crystal thin plate 120), the slope is (111), so that stress concentration can be relaxed, the reliability of the torsion spring can be improved, and the light deflection angle of the mirror can be increased.
[0094]
4). After the anisotropic etching, isotropic etching may be performed with gas or acid to round the corners of the torsion spring. In this way, stress concentration on these portions can be alleviated.
[0095]
5. Next, the mask layer 150 is removed (e).
6). Finally, the mirror 130 is cleaned, and a light reflecting film is formed on the surface.
[0096]
About the processing method of the glass substrate 110, it is the same as description of Example 1 described along FIG.
[0097]
As described above, according to the manufacturing method of the present embodiment, the torsion springs in which the torsion bars 122, 123; 124, 125 having a flat cross section are combined in an inverted C shape by performing anisotropic etching only once. 128, 129 can be manufactured.
[0098]
As shown in FIG. 18, in the torsion spring 128 (129) of the optical deflector of this embodiment, the two flat torsion bars 122 (124) and 123 (125) have an angle of 70.6 ° with respect to each other. Are arranged. That is, since the flattened torsion bar is combined so that the most flexible direction (low bending rigidity) is not parallel, the entire torsion spring has a high bending rigidity. Furthermore, since the cross-sectional shape of the torsion springs 128 and 129 has two intersecting portions inclined with respect to the plane of the flat plate-like rocking body (mirror 130), it is further perpendicular and parallel to the plane of the rocking body. The structure is difficult to bend.
[0099]
According to the present embodiment, unlike a torsion bar having a T-shaped cross section, a large stress concentration does not occur. Therefore, when considering a torsion spring having the same torsion spring constant and the same length, it is possible to realize a microstructure that is less likely to break. . Further, according to the present embodiment, when considering the same allowable torsion angle, it is possible to realize a microstructure that can be further reduced in size as compared with a torsion bar having a T-shaped cross section. Furthermore, by using single crystal silicon as a material, it is possible to realize a microstructure having a mechanical Q value larger than that of polysilicon.
[0100]
According to the present embodiment, it is possible to realize a micro optical deflector that is harder to break, can be reduced in size, and has a large vibration amplitude when driven by resonance. Furthermore, the microstructure of the present invention can be manufactured relatively easily by using the manufacturing method of this embodiment.
[0101]
A modification of the third embodiment will be described with reference to FIG. FIG. 20 is a perspective view (a) and a sectional view (b) for explaining a micro optical deflector according to a modification of the third embodiment of the present invention. In this modification, the torsion bar has a flat cross section surrounded by the substrate surface and the (111) plane of silicon, and these two are combined in a reverse C and C shape to form torsion springs 528 and 529. ing. Also in FIG. 20, the side surfaces of the reflecting surface 530 and the frame body 520 are shapes in which the (111) surface of silicon is exposed, but are drawn as side surfaces perpendicular to the reflecting surface 530 for simplicity.
[0102]
As shown in FIG. 20B, the micro optical deflector according to the present modification has a substrate surface (more precisely, the shape of the AA ′ cross section and the BB ′ cross section of the torsion bar). The surfaces are symmetrical to each other with respect to the torsion springs facing torsional central axes and parallel to the reflecting surface 530. As a result, during torsional resonance drive, unnecessary motion modes such as flexural vibrations caused by one torsion bar structure and the influence of disturbance can be canceled by the other torsion bar structure, and drive stability is improved. be able to.
[0103]
In the micro optical deflector according to this modification, anisotropic etching is performed in the same manner as in the third embodiment (only the pattern of the mask layer 150 in FIG. 19 is changed (upside down) for the other torsion bar structure). The torsion springs 528 and 529 combined with a torsion bar having a flat cross section can be easily manufactured by performing only once.
[0104]
In this modification, the process is easy, and the cross-sectional shapes of the two sets of torsion springs are different from each other, so that it is possible to cancel the influence of disturbances during driving caused by the respective torsion springs as described above. In addition, it is possible to realize a micro optical deflector having a structure in which the torsion bar has no stress concentration portion and is difficult to break.
[0105]
[Example 4]
FIG. 21: has shown the schematic perspective view for demonstrating the micro optical deflector of Example 4 of this invention. Also in the micro optical deflector of the present embodiment, the torsion spring (not shown) and the mirror 330 as described in the above embodiments or modifications are integrally formed on the silicon single crystal thin plate by bulk micromachining technology. ing. A movable core 341 made of a soft magnetic material is fixed to the end of the mirror 330. The mirror 330 has a surface coated with a material having a high light reflectivity, and is supported by a torsion spring so as to be swingable around its torsion axis, which is its long axis.
[0106]
On the other hand, a fixed core 342 made of a soft magnetic material is disposed on a glass substrate (not shown), and a coil (not shown) goes around the fixed core 342. The silicon single crystal thin plate and the glass substrate are bonded so that the substantially parallel faces of the movable core 341 and the fixed core 342 are maintained at a predetermined interval. That is, when the mirror 330 is swung, the overlapping area (the cross-sectional area where the movable core 341 cuts off the magnetic flux generated in the fixed core 342) changes while the opposing surfaces remain substantially parallel. ing. The movable core 341 and the fixed core 342 form a closed series magnetic circuit including two gaps.
[0107]
The operation of the optical deflector of this embodiment will be described.
When the coil is energized, the fixed core 342 is excited. FIG. 21 illustrates a state in which the front side of the fixed core 342 is excited to the N pole and the back side is excited to the S pole. Then, the movable core 341 is attracted in the direction in which the overlapping area of the opposing surfaces increases (the direction attracted by the magnetic flux path generated by the fixed core 342), that is, in the direction of the arrow in FIG. Since the movable core 341 and the fixed core 342 are arranged in different heights when not energized so that the overlapping area of the facing surfaces can be increased, a counterclockwise rotational moment is generated around the torsion spring. When energization of the coil is turned ON / OFF in accordance with the resonance frequency of the mirror 330, the mirror 330 resonates around the torsion spring. In this state, the light can be scanned by making the light incident on the mirror 330.
[0108]
[Example 5]
FIG. 22 is a diagram illustrating the optical scanning display according to the fifth embodiment. The X light deflector 401 and the Y light deflector 402 are the same as the light deflectors of the above-described embodiments or modifications. The controller 409 controls the X light deflector 401 and the Y light deflector 402, scans the laser beam 410 in a raster shape, and modulates the laser oscillator 405 according to the information to be displayed, whereby an image is displayed on the screen 407. Are displayed two-dimensionally.
[0109]
By applying the optical deflector of the present invention to an optical scanning display, it is possible to realize an optical scanning display that can form a fine image and has high energy efficiency.
[0110]
【The invention's effect】
As described above, according to the present invention, the cross-sectional shape of the torsion spring that supports the rocking body is formed to have a portion inclined with respect to the plane of the flat rocking body. Therefore, it is difficult to bend in the direction perpendicular to or parallel to the plane, and it is possible to effectively realize a microstructure that enables an accurate swing motion of the swing body. Further, if the material is a single crystal material, it is possible to provide a micro structure having a torsion spring which is easy to twist and is not easily bent and has a large mechanical Q value. In addition, since the mechanical Q value is high, it is possible to provide a mechanical quantity sensor with low noise and high sensitivity. Further, since the mechanical Q value is high, a microactuator having a large amplitude and high energy efficiency when driven by resonance can be provided. In addition, since the mechanical Q value is high, a micro optical deflector having a large amplitude and high energy efficiency when driven by resonance can be provided.
[0111]
By applying the optical deflector of the present invention to an optical scanning display, an optical scanning display capable of forming a fine image can be provided. Furthermore, by using the manufacturing method of the present invention, the microstructure, the micro optical deflector, the micro mechanical quantity sensor, and the micro actuator of the present invention can be manufactured relatively easily.
[Brief description of the drawings]
FIG. 1 is a perspective view for explaining an optical deflector according to a first embodiment of the present invention.
2A is an exploded view for explaining the optical deflector of Embodiment 1, and FIG. 2B is a longitudinal sectional view of the torsion bar;
FIG. 3 is a cross-sectional view for explaining an optical deflector according to the first embodiment or the like.
4 is a cross-sectional view of a torsion bar portion for explaining the optical deflector of Embodiment 1. FIG.
FIG. 5 is a diagram illustrating anisotropic etching of silicon.
6 is a diagram illustrating a process for producing a silicon single crystal thin plate of the optical deflector of Example 1. FIG.
7 is a diagram illustrating a process for producing a glass substrate of an optical deflector according to Embodiment 1 or the like.
8A is a perspective view for explaining an optical deflector according to a modification of the first embodiment of the present invention, and FIG. 8B is a sectional view of a torsion spring.
FIG. 9 is a perspective view for explaining an optical deflector according to a second embodiment of the present invention.
FIG. 10 is an exploded view (a) for explaining an optical deflector according to a second embodiment and a longitudinal sectional view (b) of a torsion spring.
FIG. 11 is a cross-sectional view of a portion of a torsion spring for explaining an optical deflector according to a second embodiment.
12 is a plan view for explaining an optical deflector according to Embodiment 2. FIG.
13 is a diagram illustrating a process for producing a silicon single crystal thin plate of the optical deflector of Example 2. FIG.
FIG. 14A is a perspective view for explaining an optical deflector according to a modification of the second embodiment of the present invention, and FIG. 14B is a sectional view of a torsion spring.
15 is a diagram illustrating a process for producing a silicon single crystal thin plate of an optical deflector according to a modification of Example 2. FIG.
FIG. 16 is a perspective view for explaining an optical deflector according to a third embodiment of the present invention.
FIG. 17 is an exploded view (a) for explaining the optical deflector of Embodiment 3, and a longitudinal sectional view (b) of the torsion spring.
FIG. 18 is a cross-sectional view of a portion of a torsion spring for explaining an optical deflector according to a third embodiment.
19 is a diagram illustrating a process for producing a silicon single crystal thin plate of the optical deflector of Example 3. FIG.
20A is a perspective view for explaining an optical deflector according to a modification of the third embodiment of the present invention, and FIG. 20B is a sectional view of a torsion spring.
FIG. 21 is a schematic perspective view illustrating the operation principle of the optical deflector according to the fourth embodiment.
FIG. 22 is a diagram illustrating an optical scanning display according to a fifth embodiment of the present invention.
FIG. 23 is a perspective view for explaining a conventional optical deflector.
FIG. 24 is an exploded view for explaining a conventional optical deflector.
FIG. 25 is a cross-sectional view for explaining a conventional optical deflector.
FIG. 26 is a cross-sectional view of a portion of a torsion bar for explaining a conventional optical deflector.
FIG. 27 is a top view illustrating a conventional hard disk gimbal.
FIG. 28 is a cross-sectional view for explaining a conventional hard disk gimbal.
FIG. 29 is a diagram for explaining a process for producing a conventional hard disk gimbal.
[Explanation of symbols]
110 Glass substrate
112 dent
114, 116 drive electrode
120, 620, 720 Silicon single crystal thin plate
122, 123, 124, 125, 128, 129, 528, 529, 628, 629, 728, 729 Torsion spring (torsion bar)
122a, 124a, 128a, 129a Slope at the base of the torsion spring
130, 330, 630, 730 Mirror
132 Mirror support
150, 731, 732 Mask layer
190, 191 opening
341 Movable core
342 fixed core
401 X light deflector
402 Y light deflector
405 Laser oscillator
407 screen
409 controller
410 Laser beam
1010 Insulating substrate
1014, 1016 Driving electrode
1020 Silicon thin plate
1022, 1024, 2001, 2002 Torsion bar
1030, 2011 Mirror
1032 Mirror support
2020 Gimbal
2022, 2024 Roll torsion bar
2026, 2028 Pitch torsion bar
2030 Head support
2031 Support frame
2091 Silicon wafer for mold making
2092 Sacrificial layer
2093 Polysilicon layer
2094 Epoxy resin
2095 pad

Claims (10)

In a microstructure having a substrate and a plate-shaped oscillating body, and the oscillating body is elastically supported by the torsion bar with respect to the substrate about the torsion axis of the torsion bar,
The substrate, the rocking body and the torsion bar are integrally formed from a single crystal material,
The torsion bar is
On each of the upper surface that is the same surface side as the surface side of the rocking body and the lower surface that is the same surface side as the back surface side, there is a groove extending in parallel to the torsion axis,
The width Wg of the groove, and the distance t between the upper surface and the lower surface, satisfy the relationship of Wg <t / tan 54.7 °, and the shape of the cross section perpendicular to the torsional axis is the X-shaped Having a cross-sectional shape,
A micro structure characterized by that. The microstructure according to claim 1, wherein the torsion shaft passes through the center of gravity of the rocking body. 2. The microstructure according to claim 1, wherein the single crystal material is single crystal silicon having a thickness t . 4. The micro of claim 3, wherein the single crystal material is a (100) substrate, and an inclined surface with respect to the (100) plane of the (100) substrate that defines an outer surface of the torsion bar is a (111) plane. Structure. The microstructure according to claim 1, wherein corners of the torsion bar are rounded. 2. The microstructure according to claim 1, wherein a plurality of the oscillators are arranged in series with the torsion bar interposed therebetween. A micro mechanical quantity sensor comprising: the microstructure according to claim 1; and a displacement detection means for detecting a relative displacement between the substrate and the oscillator. A microactuator comprising: the microstructure according to claim 1; and a driving unit that drives the rocking body relative to the substrate. 2. A micro optical deflector comprising: the microstructure according to claim 1; drive means for driving the oscillator relative to the substrate; and an optical deflector provided on the oscillator. 10. An optical scanning display comprising: the micro light deflector according to claim 9; a light source capable of modulation; and control means for controlling the modulation of the light source and the operation of an oscillator of the micro light deflector.

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