JP4566014B2 - Optical scanning apparatus and image forming apparatus - Google Patents

Description

  The present invention relates to an optical scanning device and an image forming apparatus (such as a digital copying machine or a laser printer) including the same.

  In a conventional optical scanning device, a polygon mirror or a galvanometer mirror is used as a deflector for scanning a light beam.

  An optical scanning device is mainly used for an image forming apparatus, but recent image forming apparatuses are required to form high-resolution images at high speed. For this purpose, it is necessary to rotate the polygon mirror as a deflector at high speed or to swing the galvanometer mirror at high speed. In this case, problems such as insufficient durability of the bearing, heat generation due to windage damage, and noise occur, and thus there is a limit to high-speed scanning in the optical scanning device of the conventional structure.

  On the other hand, in recent years, research on an optical deflector using silicon micromachining has been advanced. As a prior art relating to an optical polarizer using silicon micromachining, there is an “optical scanning device” disclosed in Patent Document 1.

  In an optical polarizer using silicon micromachining, as disclosed in Patent Document 2 and Patent Document 3, a method of integrally forming a vibrating mirror and a torsion beam that pivotally supports it on a Si substrate has been proposed. .

  According to the methods disclosed in Patent Document 2 and Patent Document 3, since reciprocation is performed using resonance, there is an advantage that noise is low although high-speed operation is possible. Further, since the driving force for swinging the vibrating mirror can be small, power consumption can be reduced.

In the case of a mirror that reciprocates using resonance,
(1) The resonance frequency fluctuates due to external factors (temperature, humidity, vibration, etc.), and the deflection angle becomes extremely small.
(2) Since the resonance frequency varies due to variations in shape and external factors that occur during fabrication, if the variation is large, the driving frequency must be changed when using a plurality of mirrors, which is complicated. In addition, there is a problem with respect to scanning stability, which is costly.
Furthermore, in the case of an electrostatically driven mirror that uses electrostatic force and has low power consumption,
(3) The drive voltage increases when trying to obtain a large deflection angle.
There is a problem.

  In order to solve such a problem, it is necessary to apply a large external force as a driving source stably and continuously. Patent Document 3 discloses that the fixed electrode is disposed at a position that does not overlap the vibration direction of the mirror portion, but the external force obtained as such a configuration is not sufficient.

Non-Patent Document 1 discloses a device in which the drive voltage is reduced without changing the deflection angle of the mirror by installing the counter electrode so as to be inclined from the center of the deflection of the mirror. On the other hand, Patent Document 4 discloses a configuration in which the drive voltage is lowered by giving an inclination to a vibrating mirror. In the inventions disclosed in Non-Patent Document 1 and Patent Document 4, there is a concern that when the mirror shakes greatly and the fixed electrode comes into contact, the mirror and the fixed electrode may be fixed, and there is a problem in reliability. is there.
JP 2002-48998 A Japanese Patent No. 2924200 Japanese Patent No. 30111144 JP 2001-33727 A The 13th Annual International Workshop on MEMS2000 (2000) 645-650

  The present invention has been made in view of such a problem, and an optical scanning device capable of stably rotating a mirror with a small driving voltage and absorbing a variation in resonance frequency to stably obtain a necessary deflection angle, and An object of the present invention is to provide an image forming apparatus provided with the same.

In order to achieve the above object, according to a first aspect of the present invention, there is provided a mirror substrate that deflects a light beam from a light source by reciprocally oscillating a beam as a torsional rotation axis, and the beam undergoes torsional displacement by vibration. A torsion spring portion that is generated, and a pair of connecting branch portions that branch from one end of the torsion spring portion and extend in the other end direction after branching, and then bend and extend again in one end direction to connect the mirror substrate to the peripheral portion. Bei example, connecting branch portion is to provide an optical scanning apparatus according to claim Rukoto a movable comb electrodes.

Further, Te first aspect of the configuration odor of the present invention, the substrate is, by being spatially insulated separated by a slit groove penetrating in the vertical direction relative to the plane of the mirror substrate when not vibrating, some Is a mirror substrate , and the slit groove is preferably in communication with the oscillating space of the mirror substrate . In addition to obtaining good insulation characteristics between the electrode parts due to the slit groove, the slit groove communicates with the oscillating space when the oscillating space is hermetically sealed, so the getter (gas adsorbent) is connected to the slit groove. The desired vacuum / airtight sealed space can be set and maintained.
Further, it is preferable to have drive voltage generating means for reciprocally vibrating the mirror substrate by applying a voltage of a predetermined frequency, and driving the vibrating mirror in a band near the resonance frequency and deviating from the resonance peak. By using it in a band outside the resonance peak, the adjustment range for the drive frequency can be expanded.

  According to a second aspect of the present invention, there is provided an optical scanning device according to any one of the first aspect of the present invention, a photoconductor on which an electrostatic image is formed by the optical scanning device, An image forming apparatus comprising: a developing unit that visualizes an image with toner; and a transfer unit that transfers the visualized toner image to a recording medium. With such a configuration, it is possible to obtain an image forming apparatus with low power consumption and low noise as compared with a conventional polygon mirror.

  According to the present invention, an optical scanning device capable of stably rotating a mirror with a small driving voltage and absorbing a variation in resonance frequency to stably obtain a necessary deflection angle, and an image forming apparatus including the same are provided. Can be provided.

[Principle of the Invention]
An optical scanning apparatus that suitably implements the present invention will be described. Here, an electrostatic drive type micromirror composed of two Si substrates is taken as an example, but three or more substrates may be used.
FIG. 10 shows a structure of a conventional micromirror in which the movable comb electrode has a mirror substrate end and a pair of connecting branches. This micromirror has a configuration in which a first Si substrate shown in (a) and a second Si substrate shown in (b) are joined via an insulating layer.

  FIG. 11 shows a cross section taken along the line A-A ′ of the micromirror. The micromirror is manufactured using an SOI substrate. Here, both SOI substrates use low-resistance substrates (conductors). These substrates are formed by etching so that the oscillating space of the oscillating mirror is formed on the second Si substrate, and the oscillating mirror is formed on the first Si substrate. Note that by using a low-resistance substrate (conductor), the substrate itself can be used as an electrode without forming metal on the substrate. Furthermore, the first and second fixed comb electrodes are formed on the respective substrates at positions facing the movable comb electrodes on the vibrating mirror side. By making the electrode shape into a comb shape, the driving voltage can be reduced. Further, since the electrodes are formed in two stages in the torsional rotation direction, the driving torque is always applied to the vibrating mirror, and the deflection angle is reduced. It can be taken big.

  In addition, a metal film is formed on the slit grooves, electrode pads, and mirror surfaces for insulating and separating the plurality of electrodes.

  A through hole is formed in the first Si substrate at a position facing an electrode pad formed on the second Si substrate, and serves as an electrode extraction opening. Therefore, in the illustrated configuration, the electrode pad of the electrode formed on the same substrate as the oscillating mirror and the electrode pad of the electrode formed on the other substrate are exposed in the same direction (upward in the drawing). Is formed. In addition, a getter (gas adsorbent) can be disposed in the slit groove that performs insulation separation of the SOI substrate. Since the slit groove is connected to the sealing space, a desired vacuum / airtight sealing space can be set and maintained by arranging the getter.

  FIG. 12 shows the configuration of the micromirror of the present invention in which the torsion spring portion and the connecting branch portion face each other and are manufactured using the same manufacturing method. While including a movable electrode equivalent to that in FIG. 10, an increase in the chip area is suppressed. Further, since the branch portion between the torsion spring portion and the connecting branch portion is larger than the configuration shown in FIG. 10, the torsional stress is relieved and the torsion spring is not easily damaged.

FIG. 13 shows a configuration in the case where there are a plurality of electrode portions in the horizontal and vertical directions. (A) is a top view of the first Si substrate on which the oscillating mirror is formed, and a plurality of movable electrodes formed on the mirror end part and the connecting branch part are formed at different positions from the rotation axis. Has been. FIG. 6B is a top view of a second Si substrate in which a plurality of fixed electrodes formed in the vertical direction of the vibrating mirror are independent. By adopting such a configuration, as will be described later (see FIGS. 3 to 5 and the text explaining them), driving force can be continuously applied, so that the driving voltage can be lowered. It becomes. In addition, when using in a band that deviates from the resonance peak, it is possible to suppress a rapid decrease in the swing angle, and the swing angle can be kept high (large) and stable.
Note that the electrode pads of the first substrate and the electrode pads of the second substrate are arranged at opposite positions (in other words, the slits of the first substrate and the slits of the second substrate overlap as much as possible). Not to be) By adopting such a configuration, the island-shaped fixed electrodes separated by the slits of the first and second substrates cross each other, and there is an effect that the strength of the substrate is improved.

  The operation state of the micromirror according to the present embodiment will be described.

Embodiment
FIG. 1 shows a configuration of a vibrating mirror module used in an optical scanning device according to a preferred embodiment of the present invention.
The vibrating mirror substrate is configured by joining two Si substrates 206 and 207 via an insulating film (such as an oxide film). The first Si substrate 206 is a silicon substrate having a thickness of 60 μm, and the periphery of the movable mirror 202 and the torsion beam 208 pivotally supported on the same straight line is removed from the fixed frame 210 by etching the periphery thereof. Is formed by.

  The movable mirror 202 is formed to be axially symmetric with the torsion beam 208 as an axis of symmetry, and has a comb-teeth shape so as to mesh with each other with a gap of several μm at the edge of both ends and the inner side of the opposing fixed frame 210. Asperities are formed. On the surface of the movable mirror 202, a metal film (Au or the like) is deposited to form a reflective surface.

  As shown in FIG. 2, by separating each substrate joined through an insulating layer into an island shape, the substrate itself is individually formed as an electrode, and the concave and convex portions at both ends of the movable mirror are formed in the first and second portions. The movable electrode (represented by different names for convenience of explanation but the same potential), and the concave and convex portions of the fixed frame 210 facing each other are defined as first and second fixed electrodes (represented by different names for convenience of explanation but same potential).

  In addition, the second substrate 207 is a 140 μm silicon substrate, which is etched in a serrated shape so as to penetrate the central portion by etching and to have an outline that coincides with the inner side that overlaps the uneven portion formed in the fixed frame 210. Similarly, the third and fourth fixed electrodes 211 and 212 are formed. The third and fourth fixed electrodes 211 and 212 pass so that the first and second movable electrodes are engaged with each other along the swing of the movable mirror.

  A voltage pulse having the same phase is applied to the first and second fixed electrodes 203 and 204, and the third fixed electrode 211 is advanced than the voltage pulse applied to the first and second fixed electrodes 203 and 204. A voltage pulse having a phase delayed from the voltage pulse applied to the first and second fixed electrodes 203 and 204 is applied to the fourth fixed electrode 212.

FIG. 3 shows the electrostatic torque generated between the electrodes corresponding to the deflection angle of the movable mirror. FIG. 4 shows a cross section of the electrode. In the figure, the counterclockwise electrostatic torque is positive.
The initial state of the movable mirror 202 is horizontal, but when a voltage is applied to the third fixed electrode 211, an electrostatic force is generated in the negative direction between the opposing movable electrodes, and the torsion beam 208 is rotated while being twisted. It tilts to a deflection angle that balances the restoring force of the torsion beam 208. When the voltage is released, the movable mirror 202 returns to the horizontal due to the restoring force of the torsion beam 208, but in the positive direction by applying a voltage to the first and second fixed electrodes 203 and 204 immediately before returning to the horizontal. The electrostatic force is generated and the voltage is continuously applied to the fourth fixed electrode 212, so that the electrodes are switched so as to further increase the electrostatic torque in the positive direction. By repeating this, the movable mirror is reciprocally oscillated at a deflection angle (about 2 ° in this case) that passes through the first and second fixed electrodes 203 and 204 facing the movable electrodes at both ends.

  Here, the moment of inertia of the movable mirror 203 and the width and length of the torsion beam 208 are matched with the desired drive frequency to be scanned, and the first resonance mode band with the torsion beam 208 as the rotation axis is applied. Thus, the vibration of the movable mirror is excited, the amplitude is remarkably increased, and the swing angle can be expanded to an angle through which the movable electrodes at both ends of the movable mirror pass through the opposing third and fourth fixed electrodes.

  As a result, an electrostatic force is generated in the direction of returning to the horizontal even when the deflection angle has passed through the third and fourth fixed electrodes. In the third fixed electrode, an electrostatic force is generated in the positive direction in the movable mirror. A large deflection angle can be maintained even at a drive frequency that deviates from the resonance frequency.

FIG. 5 shows the characteristic of the deflection angle with respect to the drive frequency. If the drive frequency is made to coincide with the resonance frequency, the swing angle can be maximized, but if the frequency changes near the resonance frequency, the swing angle changes sharply. Therefore, initially, the drive frequency applied to the fixed electrode in the drive control unit of the movable mirror can be set to match the resonance frequency, but when the resonance frequency fluctuates due to a temperature change or the like, the deflection angle drastically decreases. The stability over time is poor.
Further, as will be described later, in the case of a configuration having a plurality of movable mirrors, there are variations in the specific resonance frequency, and therefore it cannot be driven at a common drive frequency.

  For this reason, the drive frequency is set in the vicinity of the resonance frequency unique to the vibration part composed of the movable mirror 202 and the torsion beam 208 and in a band on the higher frequency side than the resonance frequency, in which the change of the deflection angle is relatively small. For example, if the resonance frequency is 2 kHz, the drive frequency is 2.5 kHz, and the deflection angle is adjusted to ± 5 ° by gain adjustment.

At this time, it is preferable to set the drive frequency in a frequency band in which the drive frequency does not reach the resonance frequency regardless of any variation in the resonance frequency due to the processing error of the vibration mirror and variation in the resonance frequency due to temperature.
For example, when the resonance frequency is 2 kHz, the variation in the resonance frequency due to processing errors is 300 Hz, and the variation in the resonance frequency due to temperature is 3 Hz, the drive frequency is preferably set to 2.303 KHz or more or 1.697 kHz or less.

When the dimensions of the movable mirror are the length 2a, the width 2b, the thickness d, the length of the torsion beam is L, and the width is c, the moment of inertia I and the spring are obtained using the density ρ of material Si and the material constant G. The constant K is expressed as in the following formulas (1) and (2).
I = (4abρd / 3) · a ² (1)
K = (G / 2L) · {cd (c ² + d ² ) / 12} (2)

The resonance frequency f is represented by the following formula (3).
f = (1 / 2π) · (K / I) ^1/2 = (1 / 2π) · {Gcd (c ² + d ² ) / 24LI} ^1/2 (3)

Here, since the beam length L and the deflection angle θ are in a proportional relationship, the deflection angle θ is expressed by the following equation (4).
θ = A / If ² (A is a constant) (4)
Since the deflection angle θ is inversely proportional to the inertia moment I, if the resonance frequency f is increased without reducing the inertia moment I, the deflection angle θ is reduced. For this reason, on the back side of the movable mirror reflecting surface (the back surface of 202 in FIG. 1), the portion of the substrate thickness d is left in a lattice shape, and the other portions are etched to a thickness of d / 10 or less to be thinned. Thus, the inertia moment I is reduced to about 1/5.

  These parameters that are useful for the moment of inertia, dimensional errors of the torsion beam, and the like cause variations in the resonance frequency.

On the other hand, when the dielectric constant ε of air, the electrode length is H, the applied voltage is V, and the distance between the electrodes is δ, the electrostatic force F between the electrodes is expressed by the following formula (5).
F = εHV ² / 2δ (5)
The deflection angle θ is also expressed by the following formula (6).
θ = B · F / I (B is a constant) (6)
As is clear from the equations (5) and (6), the greater the electrode length H, the larger the deflection angle θ, and the comb-teeth shape allows a driving torque 2n times the number of comb teeth n. It has gained. In this way, by increasing the outer peripheral length as much as possible to increase the electrode length, a large electrostatic torque can be obtained at a low voltage.

By the way, when the air density is η with respect to the speed u and area E of the movable mirror, the viscous resistance P of the air that works opposite to the rotation direction of the movable mirror is expressed by the following equation (7).
P = C · ηu ² · E ³ (C is a constant) (7)

Accordingly, it is preferable to hold the movable mirror in a sealed state with a cover in a reduced pressure state.
In this embodiment, a swinging space of the movable mirror is formed in a concave shape at the center of the vibrating mirror substrate formed by joining the first and second substrates 206 and 207. The oscillating mirror substrate is mounted on a base substrate 217 having lead terminals with the reflecting surface facing upward and the torsion beam aligned on a straight line connecting a pair of V grooves formed on the outer edge of the base. Further, a cover 205 made of a transparent resin formed into a cap shape is joined to the upper surface of the second substrate 207, and a non-evaporable getter is enclosed in the swing space. The non-evaporable getter is activated by heating from the outside, and the atmospheric pressure in the oscillating space is set to 133.322 Pa or less. The light beam enters and exits through a slit window 213 formed in the cover 205.

  On the inner side of the cover 205, a counter mirror is formed integrally in a direction orthogonal to the torsion beam so as to face the movable mirror 202. The two opposing mirrors 215 are inclined at predetermined angles (here, 9 ° and 26.3 °) from the substrate surface so as to form a predetermined angle (individually, 144.7 °) in a roof shape with the slit window 213 interposed therebetween. A metal film is vapor-deposited on the inclined surface, and the reflecting surfaces (215 in FIG. 1 and 402 and 403 in FIG. 6) are arranged in pairs.

  The bottom surface of the cover 205 is formed in parallel with the movable mirror surface and is in contact with and joined to the upper surface of the frame portion of the second substrate 207. At this time, the second substrate 207 is positioned to position the counter mirror. Indices 214 are drawn by etching on both sides and aligned on the substrate so that the edge of the counter mirror is aligned with this, so that the direction of the counter mirror can be accurately aligned with the main scanning direction.

  FIG. 6 shows a sub-scan section of the optical scanning device. As will be described later, the light beam emitted from the semiconductor laser 101 passes through the coupling lens 110 and the cylinder mirror 136, and is approximately within the sub-scanning direction with respect to the normal line in the sub-scanning section including the torsion beam with respect to the movable mirror 401. The light is incident from the slit window 404 at an angle of 20 °. The reflected light beam is incident on the first reflecting surface 402 and returned to the movable mirror, and the reflected light beam is incident on the second reflecting surface 403 through the slit window 404 and between the movable mirror and the movable mirror. The reflection position is moved in the sub-scanning direction while reciprocating three times, and the light is again emitted from the slit window 404 by a total of five reflections by the movable mirror.

  In the optical scanning device according to the present embodiment, the optical path is folded by repeating the reflection multiple times as described above, so that a large scanning angle can be obtained even if the swing angle of the movable mirror is small.

Now, assuming that the total number of reflections at the movable mirror is N and the deflection angle is θ, the scanning angle α is expressed as α = 2Nθ. In the illustrated example, since N = 5 and θ = 5 °, the maximum scanning angle α is 50 °, of which 35 ° is an image recording area. By utilizing resonance, the applied voltage can be weak, so heat generation is small. As is apparent from the above equation, the spring constant K of the torsion beam must be increased as the recording speed (that is, the resonance frequency) increases. The swing angle cannot be obtained.
For this reason, the scanning angle is enlarged by providing the counter mirror as described above, and a necessary and sufficient scanning angle is obtained regardless of the recording speed.

  In addition, a reflecting surface is formed facing the roof, and the incident angle in the sub-scanning direction to the movable mirror is repeatedly positive and negative for each reflection, in other words, the traveling direction accompanying reflection is distributed to the right and left. Therefore, the bending of the scanning line on the scanning surface due to the oblique incidence is suppressed, the linearity is maintained, and the rotation of the light beam in the plane orthogonal to the optical axis returns to the original posture at the time of emission. Consideration is given to avoid degradation of image performance.

FIG. 7 is an exploded perspective view of the optical scanning device according to the present embodiment. FIG. 8 shows an arrangement example of optical elements.
A semiconductor laser 101 as a light source is press-fitted into a stepped through-hole 103 provided on a wall provided upright on a frame member 102 from the opposite side with respect to the outer periphery of the stem, and a light is applied by striking the flange surface against the stepped portion. Axial positioning is performed. The U-shaped recess 105 has a light emitting point and light so that the optical axis of the coupling lens 110 is aligned with the emission axis from the semiconductor laser 101 via the UV adhesive, and the emitted light beam becomes a parallel light beam. Positioning in the axial direction is performed, and the UV adhesive in the gap between the recess and the coupling lens is cured and fixed.
In the illustrated example, there are three light source units, but all have the same configuration.

  The light beam emitted from the coupling lens is bonded to the pair of mounting slopes 109, is incident on the cylinder mirror 136 having a negative curvature in the sub-scanning direction, and vibrates as a focused light beam that is focused on the movable mirror surface in the sub-scanning direction. The light enters from the slit window of the mirror module 130.

  The oscillating mirror module 130 is positioned on the basis of the outer edge of the base from the back side of the stepped square hole 104 provided on the bottom surface side of the frame so that the direction of the torsion beam matches the optical axis direction. It is positioned according to the position of the possible mirror surface. In the configuration of the embodiment, three oscillating mirror modules are positioned by a single frame member 102 at equal intervals.

  When each vibrating mirror module is fixed to the printed circuit board 112 by inserting the lead terminals protruding from the bottom surface of the base board into the through holes and soldering, and abutting and fixing the upper surface of the board so as to close the lower opening of the frame member 102. At the same time, circuit connections are made.

  The printed circuit board 112 is mounted with a semiconductor laser drive circuit, electronic components constituting a movable mirror drive circuit, and a synchronization detection sensor 113, and wiring with external circuits is made in a lump.

  A cable 115 having one end connected to a printed circuit board is connected to a lead terminal of the semiconductor laser.

The frame member 102 is made of glass fiber reinforced resin, die-cast aluminum, or the like that can ensure rigidity to some extent, and flange portions 131 and 133 for attachment to the structure of the image forming apparatus main body are formed at both ends. The flange portion 131 has a reference hole, and the shaft portion of the fixing screw 132 is fitted to the inner diameter thereof. Moreover, the flange part 133 is provided with the long hole, and the fixing screw 132 penetrates. These are each fixed to the photosensitive member via a spring washer.
At this time, the scanning line scanned by any of the vibrating mirror modules on the surface to be scanned (photoreceptor) with the reference hole as the rotation axis is parallel to the direction x orthogonal to the moving direction y of the surface to be scanned. Adjusted to be.

  The upper surface of the frame member 102 does not have a surface parallel to the abutting surface in the mirror normal direction of each vibration module provided on the back side of the square hole 104, and protrudes from the bottom surface of the housing 106 that houses the scanning lens. The projections 135 are inserted into the engagement holes of the frame member to perform positioning on the same surface, and are installed with screws at the four corners. In the present embodiment, the screw 137 is screwed into the printed circuit board 112 through the through hole of the frame member, and is coupled in a three-piece manner so as to sandwich the frame member, and then the above-described soldering is performed.

In the housing 106, a first scanning lens 116 and a second scanning lens 117 constituting an image forming unit are arranged in the main scanning direction, and are positioned and integrally held so that the respective scanning regions slightly overlap. The
The first scanning lens 116 has a projection 120 that protrudes in the center of the reference surface in the sub-scanning direction and performs positioning in the main scanning direction, and a flat pressing surface 119 that engages both ends to perform positioning in the optical axis direction. The projections 120 are engaged with the grooves 122 formed integrally with the housing 106, the flat pressing surfaces 119 at each end are inserted into each of the pair of notches 121, and the corrugated spring 143 is used to enter the incident surface side. And the relative position of the scanning lenses is adjusted to the same plane orthogonal to the optical axis. Also, the installation height is positioned by abutting the reference surface in the sub-scanning direction against the projection 145 protruding from the housing 106 and the tip of the adjusting screw 146 that can be repeated in the sub-scanning direction, and the leaf spring 141 integrally formed with the cover 138 is positioned. Pressed and supported. The screw 147 is a screw for fixing the cover 138.

  Although the above description has been given of an example in which three optical scanning devices are arranged, the same applies regardless of the number of arrangements.

  FIG. 9 shows a configuration of an image forming apparatus including the optical scanning device according to the present embodiment. This image forming apparatus is a tandem type image forming apparatus in which four optical scanning devices 500 form an image on a corresponding photosensitive drum 504 one by one and superimpose single color images in accordance with the rotation of a transfer belt. Here, the optical scanning device is installed so that the light beam emission direction is downward.

  The transfer belt 501 is supported by a driving roller and two driven rollers, and the photosensitive drums 504 are arranged at equal intervals along the moving direction. Around the photosensitive drum, a developing roller 502 and a toner hopper 503 for supplying toner corresponding to each color of yellow, magenta, cyan, and black, and a toner remaining on the photosensitive drum after image transfer are scraped and stored with a blade. A cleaning unit 508 is integrally installed.

  For each color image, a latent image is formed by each optical scanning device 500 by using a signal from a sensor 505 that detects a registration mark formed at the end of the transfer belt 501 as a trigger and the writing timing in the sub-scanning direction is shifted. The images are sequentially superimposed on the transfer belt 501.

The paper is supplied from the paper supply tray 507 by the paper supply roller 506, sent out by the registration roller 510 in accordance with the timing of image formation of the fourth color, and transferred from the transfer belt 501 to the four colors at the same time by the transfer unit 511. The toner image is sent to the fixing device by the conveying belt 515 with the toner image placed thereon.
The transferred toner image is fixed by a fixing roller 512 and discharged to a paper discharge tray 514.

  In addition, the said embodiment is an example of suitable implementation of this invention, This invention is not limited to this, A various deformation | transformation is possible.

It is a figure which shows the structure of the vibration mirror module of the optical scanning device which concerns on suitable embodiment of this invention. It is a figure which shows the structure of the board | substrate which comprises a vibration mirror module. It is a figure which shows the relationship between the electrostatic torque of a fixed electrode, and a deflection angle. It is a figure which shows the cross section of an electrode. It is a figure which shows the relationship between a drive frequency and a deflection angle. It is a figure which shows the cross section of the subscanning direction of an optical scanning device. It is a disassembled perspective view of an optical scanning device. It is a figure which shows the example of arrangement | positioning of an optical element. 1 is a diagram illustrating a configuration of an image forming apparatus including an optical scanning device. It is a figure which shows the structure of the conventional type micromirror. It is a figure which shows the manufacturing process of a micromirror. It is a figure which shows the structure of the board | substrate which comprises the vibration mirror module concerning suitable embodiment of this invention. It is a figure which shows another structure of the board | substrate which comprises a vibration mirror module.

Explanation of symbols

DESCRIPTION OF SYMBOLS 101 Semiconductor laser 102 Frame member 103 Through-hole 104 Square hole 105 Recessed part 106 Housing 109 Mounting slope 110 Coupling lens 112 Printed circuit board 113 Synchronization detection sensor 115 Cable 116 1st scanning lens 117 2nd scanning lens 119 Flat pushing surface 120, 135, 145 Projection 121 Notch 122 Groove 130 Vibration mirror module 131, 133 Flange portion 132 Fixing screw 136 Cylinder mirror 137, 147 Screw 138 Cover 141 Leaf spring 143 Wave leaf spring 146 Adjustment screw 202 Movable mirror 203 First fixed electrode 204 First Two fixed electrodes 205 Cover 206 First substrate 207 Second substrate 208 Torsion beam 210 Fixed frame 211 Third fixed electrode 212 Fourth fixed electrode 213, 404 Slit window 214 Index 215 Opposing mirror 217 Base substrate 401 Movable mirror 402, 403 Reflecting surface 500 Optical scanning device 501 Transfer belt 502 Developing roller 503 Toner hopper unit 504 Photoconductor drum 505 Sensor 506 Paper feeding roller 507 Paper feeding tray 508 Cleaning unit 510 Registration roller 511 Transfer section 512 Fixing roller 514 Paper discharge tray 515 Conveying belt

Claims (5)

Having a mirror substrate that deflects the light beam from the light source by reciprocatingly vibrating the beam as a torsional rotation axis;
The beam includes a torsion spring portion that generates a torsional displacement due to vibration, and branches from one end of the torsion spring portion, and extends in the direction of the other end of the one end after the branching. Bei example a pair of connecting branch portion connecting the mirror substrate and the peripheral portion,
Before SL connecting branch includes an optical scanning device according to claim Rukoto a movable comb electrodes. The optical scanning apparatus according to claim 1, characterized in that it comprises an external force generating means for rotating the mirror substrate as the center axis of the front Symbol torsion spring unit. When the substrate is spatially insulated and separated by a slit groove penetrating in a direction perpendicular to the plane of the mirror substrate when not vibrating, a part of the substrate forms the mirror substrate,
The optical scanning device according to claim 1, wherein the slit groove communicates with a swinging space of the mirror substrate . Drive voltage generating means for applying a voltage of a predetermined frequency to reciprocally vibrate the mirror substrate;
4. The optical scanning device according to claim 1, wherein the mirror substrate is driven in a band near a resonance frequency and deviating from a resonance peak . 5. The optical scanning device according to claim 1, a photosensitive member on which an electrostatic image is formed by the optical scanning device, a developing unit that visualizes the electrostatic image with toner, and visualization. An image forming apparatus comprising: transfer means for transferring the toner image to a recording medium.

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