JP5470347B2 - Optical scanning device and image forming apparatus using the same - Google Patents

Description

  The present invention relates to an optical scanning apparatus including a deflecting body that deflects and scans a light beam emitted from a light source while sine-oscillating around an axis of an oscillation axis, and an image forming apparatus using the same.

  2. Description of the Related Art Conventionally, in an optical scanning device used in a laser printer, a copying machine, or the like, a MEMS (Micro Electro Mechanical Systems) mirror is used as a deflecting body that deflects and scans a light beam emitted from a light source. The MEMS mirror has a swing axis perpendicular to the normal line of the mirror, and is driven so as to reciprocally swing back and forth around the axis of the swing axis, whereby a predetermined amount on the photosensitive drum (scanned surface) is obtained. The laser beam is scanned in the scanning range.

  As a driving method of the MEMS mirror, there are a sine oscillation method in which the MEMS mirror is simply sine-wave oscillated, and a superposition driving method in which a vibration in which a sine wave having an integer multiple of the basic sine wave is superimposed is applied to the MEMS mirror. . In the sine drive method, the MEMS mirror is configured with a simple configuration in which the mirror portion is supported by a torsion bar (oscillation shaft), and the mirror portion is reciprocally oscillated with a predetermined basic sine wave around the torsion bar axis. Is done.

  In an image forming apparatus using a MEMS mirror as a deflecting body, it is necessary to assemble the MEMS mirror with high accuracy in the housing of the optical scanning device in order to prevent image degradation caused by a shift in scanning position. The MEMS mirror does not rotate continuously like a polygon mirror, but reciprocally swings around the axis of the swing axis, so that the center of the swing angle of the MEMS mirror and the optical axis of the imaging optical system of the laser beam are set. Must match. Patent Documents 1 to 5 disclose techniques relating to an adjustment mechanism that makes the center of the deflection angle coincide with the optical axis. The coincidence adjustment of the MEMS mirror and the imaging optical system by the adjustment mechanism is performed at the time of assembling and manufacturing the optical scanning device.

Japanese Patent Laid-Open No. 9-80348 JP 7-281115 A Japanese Patent Laid-Open No. 2-64521 JP-A-9-179053 JP 2007-178818 A

  However, since the adjustment as described above requires extremely high accuracy, time and skill are required, which increases the manufacturing cost of the optical scanning device. Further, since it is necessary to equip the adjusting mechanism in the housing of the optical scanning device, there is a problem that the optical scanning device is increased in size.

  The present invention has been made in view of the above circumstances, and an object of the present invention is to reduce the manufacturing cost and reduce the size of an optical scanning device including a deflecting body driven by a sine rocking method.

  An optical scanning device according to one aspect of the present invention includes a light source that emits a light beam, a control unit that controls light emission timing of the light source, and a swing shaft, and a predetermined swing angle around the swing shaft. A deflector that reflects and deflects and scans a light beam emitted from the light source while sine oscillating at a position, a driving unit that drives the deflector, and an optical axis, and the deflected and scanned light beam is scanned. An imaging optical system that forms an image on the top, and a storage unit that stores a rotational deviation amount of a center of a deflection angle of the deflector with respect to an optical axis of the imaging optical system. A first timing for starting irradiation of the light beam on the surface to be scanned with respect to a scanning line and a second timing for performing irradiation of the light beam on each scanning position on the main scanning line are set as the rotation shift amount. Control the emission timing by correcting accordingly That.

  According to this configuration, the position of the swing shaft is not mechanically adjusted so that the center of the deflection angle of the deflector coincides with the optical axis of the imaging optical system. Thus, by correcting the first timing for starting the irradiation of the light beam on the surface to be scanned and the second timing for performing the irradiation of the light beam on each scanning position on the main scanning line, the influence of the rotational deviation is corrected. to erase. Therefore, an adjustment mechanism for adjusting the rotation of the swing shaft can be omitted.

  In the above-described configuration, the deflecting body includes a mirror portion that reflects the light beam, and a torsion bar that is disposed on the swing shaft and supports the mirror portion, and the driving unit predetermines the mirror portion. The sine wave can be made to swing.

  According to this configuration, the deflecting body is configured by a so-called sinusoidal MEMS mirror. Therefore, it is possible to easily construct a mechanism for deflecting and scanning the light beam emitted from the light source while sine-oscillating around the axis of the oscillation axis at a predetermined oscillation angle.

  In this case, the first rotation adjusting mechanism further rotates the deflecting body around the axis of the first axis along the normal line of the mirror portion, and adjusts the rotational position of the deflecting body around the axis of the first axis. And a second rotation adjustment for adjusting the rotational position of the deflector around the axis of the second axis by rotating the deflector around the axis of the second axis orthogonal to the first axis and the swing axis. And a mechanism.

  According to this configuration, the other two axes (first axis and second axis) orthogonal to the swing axis can be adjusted by the first and second rotation adjusting mechanisms. Therefore, the influence of the rotational shift amount can be reliably erased only by correcting the first and second timings.

  In the above configuration, the holding mechanism for prohibiting the mirror portion from swinging around the swing shaft when the rotation position is adjusted by the first rotation adjustment mechanism and the second rotation adjustment mechanism. It is desirable to provide.

  According to this configuration, when the rotational position is adjusted by the first and second rotation adjusting mechanisms, the mirror unit is prohibited from swinging by the holding mechanism. Therefore, the rotational position adjustment of the swing shaft can be made dependent only on the correction of the first and second timings.

  In the above configuration, the first optical sensor that is disposed on the scanning start side of the main scanning line and detects a light beam emitted from the light source, and is disposed on the scanning end side of the main scanning line and is emitted from the light source. A second optical sensor for detecting a light beam, wherein the driving means is configured to perform the deflection based on a parameter depending on a time interval of a timing at which the first light sensor and the second light sensor sequentially detect the light beam. Preferably, the time interval is corrected according to the amount of rotational deviation, and the deflecting body is driven based on a correction parameter derived according to the corrected time interval.

  According to this configuration, the time interval of the timing at which the first optical sensor and the second optical sensor sequentially detect the light beam, that is, the deflection angle of the deflecting body can be corrected in consideration of the amount of rotational deviation. it can.

  An image forming apparatus according to another aspect of the present invention includes an image carrier that carries an electrostatic latent image, and the above-described optical scanning device that irradiates a light beam with a peripheral surface of the image carrier as the scanned surface. .

  According to the present invention, an adjustment mechanism for adjusting the rotation of the swing shaft of the deflecting body can be omitted. Therefore, it is possible to reduce the manufacturing cost and the size of the optical scanning device including the deflecting body driven by the sine swing method, and thus the image forming apparatus.

1 is a cross-sectional view illustrating a schematic configuration of a printer according to an embodiment of the present invention. It is a top view which shows the structure of the main scanning cross section of an optical scanning device. (A) is a figure which shows the structure of a MEMS mirror schematically, (B) is a schematic diagram which shows the relationship between the deflection angle of a MEMS mirror, and an optical axis. It is a figure which shows the structure of a MEMS mirror. It is a graph which shows the relationship between the rotation shift | offset | difference of the rocking | fluctuation axis | shaft of a MEMS mirror, and the shift | offset | difference of the writing position with respect to the to-be-scanned surface by scanning light. It is a graph which shows the relationship between the rotation gap | deviation of the rocking | fluctuation axis | shaft of a MEMS mirror, and the deviation | shift of a scanning position. It is a graph which shows the deviation | shift amount derived | led-out from the graph of FIG.5 and FIG.6 from the target value. It is a top view which shows the state which assembled | attached the adjustment jig to the optical scanning device, in order to obtain | require the amount of rotation shifts of the rocking | fluctuation axis | shaft of a MEMS mirror. It is a top view which shows the attachment state to the housing of a MEMS mirror. FIG. 10 is a side view of FIG. 9. It is a graph which shows the time interval of a BD signal. It is a graph which shows the time interval of a BD signal. 1 is a block diagram illustrating an electrical configuration of an image forming apparatus according to an embodiment.

  Hereinafter, an optical scanning device according to an embodiment of the present invention will be described with reference to the drawings. FIG. 1 is a cross-sectional view schematically showing a configuration of an image forming apparatus 1 including an optical scanning device 11 according to an embodiment of the present invention. The image forming apparatus 1 includes an optical scanning device 11, a developing device 12, a charger 13, a photosensitive drum 14 (image carrier), a transfer roller 15, a fixing device 16, and a paper feed cassette 17.

  The photosensitive drum 14 is a cylindrical member, and an electrostatic latent image and a toner image are formed on the peripheral surface thereof. The photosensitive drum 14 receives a driving force from a motor (not shown) and is rotated in the clockwise direction in FIG. The charger 13 charges the surface of the photosensitive drum 14 substantially uniformly.

  The optical scanning device 11 includes a light source such as a laser diode, a deflecting body, a scanning lens, an optical element, and the like, and is applied to the peripheral surface (scanned surface) of the photosensitive drum 14 that is substantially uniformly charged by the charger 13. Then, a laser beam corresponding to the image data is irradiated to form an electrostatic latent image of the image data. The optical scanning device 11 will be described in detail later.

  The developing device 12 supplies toner to the peripheral surface of the photosensitive drum 14 on which the electrostatic latent image is formed, thereby forming a toner image. The developing device 12 includes a developing roller that carries toner and a screw that stirs and conveys the toner. The toner image formed on the photosensitive drum 14 is transferred from the sheet feeding cassette 17 to the recording paper conveyed through the conveyance path P. The developing device 12 is supplied with toner from a toner container (not shown).

  A transfer roller 15 is disposed below the photosensitive drum 14 so as to face each other, and a transfer nip portion is formed by both. The transfer roller 15 is made of a conductive rubber material or the like and is given a transfer bias to transfer the toner image formed on the photosensitive drum 14 onto the recording paper.

  The fixing device 16 includes a fixing roller 160 having a built-in heater and a pressure roller 161 provided at a position facing the fixing roller 160, and is formed on the recording paper by heating and conveying the recording paper on which the toner image is formed. The toner image is fixed.

  Next, an image forming operation of the image forming apparatus 1 will be briefly described. First, the surface of the photosensitive drum 14 is charged almost uniformly by the charger 13. The peripheral surface of the charged photosensitive drum 14 is exposed by the optical scanning device 11, and an electrostatic latent image of an image formed on the recording paper is formed on the surface of the photosensitive drum 14. The electrostatic latent image is made visible as a toner image by supplying toner from the developing device 12 to the peripheral surface of the photosensitive drum 14. On the other hand, the recording paper is fed from the paper feed cassette 17 to the transport path P. The toner image is transferred to the recording paper when the recording paper passes through the nip portion between the transfer roller 15 and the photosensitive drum 14. After this transfer operation is performed, the recording paper is conveyed to the fixing device 16 and the toner image is fixed to the recording paper.

  Next, the detailed structure of the optical scanning device 11 will be described. FIG. 2 is a plan view showing the configuration of the main scanning section of the optical scanning device 11. The optical scanning device 11 includes a semiconductor laser 21 (light source), a collimator lens 22, a cylindrical lens 23, a MEMS mirror 24 (deflector), a first scanning lens 25, a second scanning lens 26, a first BD (Beam Detect) lens 27, A second BD lens 28, a first BD sensor 31, and a second BD sensor 32 are provided. In FIG. 2, the x axis is the direction in which the swing axis 24S of the MEMS mirror 24 extends, the y axis is the direction in which the mirror plane extends, and the z axis is the normal direction (optical axis direction) of the mirror plane.

  The semiconductor laser 21 is a light source that emits laser light having a predetermined wavelength (incident light beam L1). The collimator lens 22 converts the incident light beam L1 emitted from the semiconductor laser 21 and diffusing into parallel light. The cylindrical lens 23 converts the incident light beam L1 of the parallel light into linear light that is long in the main scanning direction and forms an image on the MEMS mirror 24. The semiconductor laser 21, the collimator lens 22, and the cylindrical lens 23 constituting the incident optical system of the incident light beam L1 with respect to the MEMS mirror 24 are arranged on the peripheral surface 14a (scanned surface) of the photosensitive drum 14 from the MEMS mirror 24 in the main scanning plane. The MEMS mirror 24 is disposed in an oblique direction so as not to intersect with the reflected reflected light beam (the deflected light beam L2). The incident optical system may be a so-called center incident optical system arranged in a sub-scan section including the optical axis.

  As shown in FIG. 3A, the MEMS mirror 24 has a mirror surface 24M and a swing shaft 24S parallel to the sub-scanning direction. As shown in FIG. 3B, the MEMS mirror 24 reciprocally swings within the range of a predetermined swing angle α around the swing shaft 24S and forms an image on the mirror surface 24M through the incident optical system. The incident light beam L1 is deflected and scanned. That is, the reflected light beam of the MEMS mirror 24 becomes the deflected light beam L2.

  The first scanning lens 25 and the second scanning lens 26 are lenses having substantially fθ characteristics that scan on the image surface at substantially constant speed, and have a lens surface (rotationally asymmetric refracting surface) formed of a special toric surface. It is a lens. These scanning lenses 25 and 26 are arranged to face each other on the optical axis from the MEMS mirror 24 toward the circumferential surface 14 a of the photosensitive drum 14. The first and second scanning lenses 25 and 26 collect the deflected light beam L2 reflected by the MEMS mirror 24 and form an image on the peripheral surface 14a.

  The first BD sensor 31 (first optical sensor) and the second BD sensor 32 (second optical sensor) are installed outside the effective scanning area of the deflected light beam L2, and the deflected light beam L2 on the peripheral surface 14a with respect to one main scanning line. The polarized light beam L2 is detected in order to synchronize the writing start timing, which is the timing for starting the irradiation. The first BD sensor 31 is disposed on the scanning start side of the main scanning line, and the second BD sensor 32 is disposed on the scanning end side of the main scanning line.

  The first BD lens 27 is a lens that is disposed in the optical path between the MEMS mirror 24 and the first BD sensor 31 and forms an image of the deflected light beam L2 on the first BD sensor 31. The second BD lens 28 is a lens that is disposed in the optical path between the MEMS mirror 24 and the second BD sensor 32 and forms an image on the second BD sensor 32 with the deflected light beam L2.

  FIG. 4 is a diagram illustrating a configuration of the MEMS mirror 24. The MEMS mirror 24 is a sinusoidal mirror, and includes a MEMS substrate 240 in which mechanical drive components are mounted on a semiconductor substrate such as silicon, and a mirror unit 241 that reflects a light beam (a member including the mirror surface 24M). And a pair of torsion bars 242 arranged so as to sandwich the mirror part 241 on the axis of the swing shaft 24S and supporting the mirror part 241. The MEMS substrate 240 is provided with a rectangular window 240W, and a torsion bar 242 is held on the inner periphery of the window 240W.

  A coil that can be energized from the outside is mounted on the mirror unit 241. A magnet is mounted on the MEMS substrate 240. An alternating current is applied to the coil, and the mirror portion 241 swings around the axis of the torsion bar 242 by a Lorentz force generated by the current and the magnetic field of the magnet. This fluctuation depends on the frequency of the applied AC voltage.

  In the present embodiment, the MEMS mirror 24 is driven by a sine swing method. Accordingly, a basic sine wave voltage having a predetermined frequency is applied to the coil of the mirror unit 241. By applying this sine wave voltage, the mirror portion 241 swings around the swing shaft 24S, and the incident light beam L1 can be deflected and scanned. The sinusoidal oscillation type MEMS mirror 24 can be simplified in configuration as compared with the superimposed drive method, but is inferior to the superimposed drive method in terms of oscillation with a constant angular velocity motion because it is driven with a sinusoidal voltage.

  The MEMS mirror 24 needs to be assembled in the housing of the optical scanning device 11 in a state where the x-axis, y-axis, and z-axis are precisely aligned and adjusted. For example, as the displacement of the x-axis swing shaft 24S, in addition to the inclination with respect to the sub-scanning direction and the parallel axis displacement, a rotational axis displacement (hereinafter referred to as “x-axis rotation”) is regarded as a problem. When the x-axis rotation exists, as shown in FIG. 3B, the optical axis of the imaging optical system in which the center αc of the deflection angle α of the MEMS mirror 24 (mirror unit 241) extends from the MEMS mirror 24 to the peripheral surface 14a. It is shifted by Δθx with respect to OA. This Δθx is the amount of rotational deviation caused by the x-axis rotation.

  The influence of the x-axis rotation will be described using the deflection angle characteristics of the MEMS mirror 24 and the characteristics of the scanning lenses 25 and 26. The deflection angle characteristic of the sinusoidal oscillation type MEMS mirror 24 is expressed by the following equation (1).

In the above equation (1), A ₀ includes the optical axis of the reflected light (= center αc of the deflection angle α) and the first and second scanning lenses 25 and 26 when the MEMS mirror 24 is stationary. x-axis rotation angle formed between the optical axis of the image optical system (Δθx), a ₁ is the maximum deflection angle of the fundamental sine wave, theta is the deflection angle of the MEMS mirror 24, omega and the angular velocity of the MEMS mirror 24, t indicates time. In the imaging optical system of the sine oscillation system, the scanning lenses (first and second scanning lenses 25 and 26) have the characteristics shown by the following equation (2).

In the above equation (2), y represents the image height, and f represents the focal length of the scanning lens. When the x-axis rotation occurs, the writing timing shift and the scanning position shift occur. FIG. 5 shows the writing position corresponding to the writing timing shift in the case where x-axis rotation exists, that is, when A ₀ ≠ 0 in the expression (1) (exposure by the deflected light beam L2 in one main scanning line). FIG. 6 is a graph showing the scanning position deviation with reference to the writing position. FIG. 6 is a graph showing the deviation amount R1 of the position on the scanning surface where (writing) is started. In FIG. 6, the scanning position deviation is shown for each of the six x-axis rotation angles a to f, and the x-axis rotation angles are a = 0 °, b = 0.0005 °, c = 0.01 °, d = 0.02 °, e = 0.03 °, and f = 0.04 °. The parameters in the equations (1) and (2) were f = 200 mm, ω = 4000πHz · rad, and A ₁ = 42.02 °. The effective scanning area is set to ± 105 mm, and the light beam detection position by the BD sensor is set to −120.95 mm.

  The threshold value Th = 42 μm displayed in FIG. 5 and FIG. 6 is a threshold value indicating an allowable range of the deviation of the writing position and the scanning position. This is because when the pixel density is 600 dpi, the size of one dot is 42 μm, and a deviation exceeding this is visually noticeable.

  As shown in FIG. 5, when the x-axis rotation exists, the writing position shift occurs, and the shift increases monotonously as the x-axis rotation angle increases. The scanning position deviation shown in FIG. 6 represents how much deviation occurs in the main scanning direction with respect to the writing position. Naturally, at the scanning position of −105 mm which is the writing position, the scanning position deviation = 0 μm.

  As apparent from FIGS. 5 and 6, the deviation of the writing position and the scanning position caused by the occurrence of the x-axis rotation are considerably large. That is, when the x-axis rotation angle is about 0.08 ° or more, the deviation R1 of the writing position exceeds the threshold Th (within 1 dot). As for the scanning position deviation, the maximum value of the scanning position deviation curve f having the x-axis rotation angle of 0.04 ° exceeds the threshold Th. When the size of the MEMS substrate 240 in the main scanning direction is 30 mm, when the x-axis rotation angle = 0.04 ° and the x-axis rotation angle = 0.08 are converted into dimensional variation amounts, they are 20 μm and 40 μm, respectively. It is difficult to suppress dimensional variations within these ranges. In conclusion, it can be said that the x-axis rotation is sensitive to both the write position shift (write timing shift) and the scan position shift.

  FIG. 7 is a diagram in which the scan position shift shown in FIG. 6 is replaced so that the x-axis rotation angle is a variable on the horizontal axis, and both the write position shift and the scan position shift are represented on the same graph. In FIG. 7, R1 represents the amount of deviation of the writing position, and R2 represents the amount of deviation of the scanning position. The sum of the deviation amount R1 at the writing position and the deviation amount R2 at the scanning position is relative to the reference position on the surface to be scanned where the deflected light beam L2 is to be originally irradiated (the coordinates thereof are “target values”). The amount of deviation R3 of the position on the surface to be scanned which the deflected light beam L2 is actually irradiated becomes.

  By obtaining the deviation amount R3, the x-axis rotation amount of the MEMS mirror 24 can be obtained. That is, after adjusting the beam diameter and the amount of light, the deflected light beam L2 is actually irradiated to a predetermined position on the surface to be scanned (for example, the center position of the scanning region), and the deflected light beam L2 is applied to the target value on the surface to be scanned. By measuring how much the position of the center of gravity of the beam spot is shifted, the amount of x-axis rotation can be measured.

  As shown in FIG. 5, the deviation of the writing position is linearly increased with respect to the x-axis rotation amount. Further, as shown in FIG. 6, the shift of the scanning position has a certain tendency with respect to the x-axis rotation amount. Therefore, even if the x-axis rotation adjustment of the MEMS mirror 24 is not actually performed, the effect of the x-axis rotation is corrected by correcting the partial equal magnification corresponding to the writing timing and the scanning position deviation according to the x-axis rotation amount. Can be erased.

  Table 1 shows an example of the correction amount of the writing start timing with respect to the x-axis rotation amount, and Table 2 shows an example of the correction amount of partial equality (scanning position deviation) with respect to the x-axis rotation amount.

  When the optical scanning device 11 is manufactured, the x-axis rotation amount is measured based on the deviation amount R3, and the write timing and partial equality correction values are stored in a memory or the like based on the tables in Tables 1 and 2. By doing so, the work for adjusting the x-axis rotation can be omitted.

Next, an example of assembly work of the optical scanning device 11 according to this embodiment will be described for each process.
[Step 1]
An adjustment jig 40 for adjusting the scanning light is attached at a position facing the photosensitive drum 14 in the housing of the optical scanning device 11. FIG. 8 is a plan view showing a state in which the adjustment jig 40 is assembled to the optical scanning device 11 in order to obtain the x-axis rotation amount of the swing shaft 24S of the MEMS mirror 24. FIG. The adjustment jig 40 includes an image forming surface (surface simulating the surface to be scanned) 40S on which the deflected light beam L2 is imaged, and the first jig BD sensor 33 and the second jig disposed on the image forming surface 40S. And a first CCD sensor 41, a second CCD sensor 42, and a third CCD sensor 43 which are two-dimensional area sensors.

  The first jig BD sensor 33 is disposed on the writing start side, the second jig BD sensor 34 is disposed outside the effective scanning area on the writing end side, and the BD sensors 33 and 34 detect the deflected light beam L2. The positions of the first and second jig BD sensors 33 and 34 in the adjustment jig 40 are known, and therefore the respective image heights on the imaging surface 40S are also known. Therefore, the angle θBD1 formed by the optical axis (image height = 0 mm) and the deflected light beam L2 incident on the first jig BD sensor 33, and the deflected light beam L2 incident on the optical axis and the second jig BD sensor 34. The angle .theta.BD2 formed by can be calculated.

  The first CCD sensor 41 is disposed at the center of the image height (image height = 0 mm), the second CCD sensor 42 is disposed at the image height end on the writing start side, and the third CCD sensor 43 is disposed at the image height end on the writing end side. The CCD sensors 41, 42, 43 detect the beam spot of the deflected light beam L2 two-dimensionally. These CCD sensors 41, 42 and 43 are installed for measuring the beam diameter of the deflected light beam L2 and detecting the light quantity. The beam diameter can be obtained by enveloping a region where light is detected on the light receiving surface. The amount of light can be obtained based on the area of the beam spot on the light receiving surface in a state where the optical system is adjusted so that the beam diameter is minimized. This is because the light amount distribution of the beam spot formed on the light receiving surface is a Gaussian distribution, and the size of the beam spot changes in proportion to the light amount.

[Step 2]
A semiconductor laser 21 as a light source and a collimator lens 22 are installed in a housing (not shown) of the optical scanning device 11. At this stage, the cylindrical lens 23, the MEMS mirror 24, and the first and second scanning lenses 25 and 26 are not attached to the housing.

[Step 3]
The driver of the semiconductor laser 21 (LD driving unit 21D in FIG. 13) is operated to turn on the semiconductor laser 21.

[Step 4]
The optical axis of the incident optical system with respect to the MEMS mirror 24 is adjusted. That is, the optical axes of the semiconductor laser 21 and the collimator lens 22 are adjusted, and the optical axis of the incident light beam L1 is adjusted to a specified position. As a result, parallel light (incident light beam L1) having a spot diameter of about 5 mm is emitted from the collimator lens 22 along the optical axis.

[Step 5]
The MEMS mirror 24 is attached to a predetermined position of the housing of the optical scanning device 11. After attachment, rotation adjustment about the y-axis and the z-axis shown in FIG. 8 is performed. As described above, the rotation adjustment of the x-axis that is the extending direction of the swing shaft 24S of the MEMS mirror 24 is not performed in this embodiment. The y axis is the direction in which the mirror plane of the MEMS mirror 24 (mirror unit 241) extends, and the z axis is the normal direction of the mirror plane.

  The optical scanning device 11 according to the present embodiment includes a support mechanism for the MEMS mirror 24 shown in FIGS. 9 and 10 in order to adjust the rotation about the y-axis and the z-axis. The support mechanism includes a pair of holding plates 51 that are part of the housing of the optical scanning device 11, and pressing protrusions 52 (holding mechanisms) that protrude from the holding plate 51. The pair of holding plates 51 are disposed at positions that cover both sides of the MEMS substrate 240 in the y-axis direction. The pressing protrusion 52 abuts on the MEMS substrate 240 on the y-axis extension line and presses the MEMS substrate 240. The MEMS substrate 240 is pressed against the wall surface of the housing facing the holding plate 51 by the pressing, and is thereby fixed to the housing.

  The MEMS substrate 240 is rotated around the y-axis and / or z-axis as necessary while being held by the support mechanism as described above, and the rotation is adjusted. Since the pressing protrusion 52 presses the MEMS substrate 240 on the y-axis extending line, the MEMS substrate 240 can rotate around the y-axis axis as shown in FIG. On the other hand, the MEMS substrate 240 cannot be rotated around the x-axis axis due to the restraint by the pair of pressing protrusions 52, and the x-axis rotation adjustment cannot be physically performed. As shown in FIG. 9, the rotation adjustment around the z-axis is an adjustment for rotating the MEMS substrate 240 in the plane of arrangement of the substrate, and therefore can be executed even in a state of being pressed by the pressing protrusion 52. it can.

[Step 6]
Using the first CCD sensor 41 arranged at the center of the image height, rotation adjustment (pitch direction adjustment) around the y-axis of the MEMS mirror 24 is performed. When the MEMS mirror 24 is not driven, the deflected light beam L2 emitted from the semiconductor laser 21 and reflected by the MEMS mirror 24 reaches the light receiving surface of the first CCD sensor 41. Since the scanning lenses 25 and 26 are not assembled at this stage, the parallel light emitted from the collimator lens 22 is received by the first CCD sensor 41. The difference between the coordinates of the irradiation position of the parallel light on the light receiving surface and a predetermined target value in the x-axis direction is the y-axis rotation amount.

  When the MEMS mirror 24 is assembled with no vibration in the pitch direction with respect to the reference position, the coordinates of the irradiation position of the linear light coincide with the target value in the x-axis direction, but there is vibration in the pitch direction. If so, they will not match. In this case, the predetermined position is set so that the irradiation position of the linear light coincides with the target value, that is, the linear light is detected from the pixels of the first CCD sensor 41 located at coordinates corresponding to the target value. The rotation mechanism (second rotation adjustment mechanism) rotates the MEMS mirror 24 (MEMS substrate 240) about the y-axis.

[Step 7]
The MEMS mirror 24 is driven to oscillate about the axis of the oscillating shaft 24S, and the rotation adjustment about the z axis of the MEMS mirror 24 is performed by using the second and third CCD sensors 42 and 43 respectively disposed at the image height end portions. Adjust the yaw direction). By driving the MEMS mirror 24, the deflected light beam L2 can reach the light receiving surfaces of the second and third CCD sensors 42 and 43. Accordingly, the irradiation position of the linear light at both ends of the image height of the deflected light beam L2 can be obtained based on the outputs of the second and third CCD sensors 42 and 43.

  When the MEMS mirror 24 is assembled in a yaw direction with respect to the reference position, for example, in the second CCD sensor 42, the irradiation position of the linear light of the deflected light beam L2 is in the + direction with respect to the target value in the x-axis direction. The third CCD sensor 43 detects the difference in the negative direction with respect to the target value. In such a case, the MEMS mirror 24 is rotated around the z-axis by a predetermined rotation mechanism (first rotation adjustment mechanism) so that the irradiation position of the linear light coincides with the target value.

[Step 8]
The cylindrical lens 23, the first scanning lens 25, and the second scanning lens 26 are attached to predetermined positions of the housing of the optical scanning device 11. Thereby, an imaging optical system from the MEMS mirror 24 to the peripheral surface 14a is constructed.

[Step 9]
The first CCD sensor 41 is used to adjust the beam diameter and the light amount of the deflected light beam L2. By assembling the first and second scanning lenses 25 and 26, the deflected light beam L2 emitted from the semiconductor laser 21 and reflected by the MEMS mirror 24 can be imaged on the light receiving surface of the first CCD sensor 41. The first CCD sensor 41 detects an image of the beam spot of the deflected light beam L2.

  The adjustment of the beam diameter is an adjustment that minimizes the beam diameter of the beam spot. For this adjustment, the positions of the collimator lens 22 and the cylindrical lens 23 of the incident optical system are adjusted while monitoring the image of the beam spot obtained from the first CCD sensor 41. The collimator lens 22 and the cylindrical lens 23 are fixed to the housing at a position where the beam diameter is minimum.

  The light amount adjustment is an adjustment so that the beam spot has a predetermined area. For this adjustment, the output adjustment of the semiconductor laser 21 is performed while monitoring the image of the beam spot obtained from the first CCD sensor 41. Since the light quantity distribution of the beam spot is a Gaussian distribution, the area of the beam spot increases in proportion to the light quantity under the condition that the above-mentioned adjustment for minimizing the beam diameter is performed. The amount of light emitted by the semiconductor laser 21 is adjusted so that the deflected light beam L2 forms a beam spot having a predetermined area on the light receiving surface of the first CCD sensor 41.

[Step 10]
The first CCD sensor 41 is used to measure the amount of rotation of the MEMS mirror 24 about the x axis (the amount of rotational displacement in the rolling direction). When the MEMS mirror 24 is not driven, the deflected light beam L2 forms an image on the light receiving surface of the first CCD sensor 41. Since the y-axis and z-axis rotation adjustment has already been performed in steps 6 and 7 above, and the beam diameter adjustment and light amount adjustment of the deflected light beam L2 have also been performed in step 9 above, the remaining error factor is only the x-axis rotation. is there. The center of gravity of the beam spot of the deflected light beam L2 imaged on the light receiving surface of the first CCD sensor 41 is defined as the beam irradiation position, and the difference between the coordinates of the beam irradiation position and a predetermined target value is measured. As described above, since the light amount distribution of the beam spot is a Gaussian distribution, the position of the center of gravity is the coordinate position of the pixel detecting the highest light amount in the first CCD sensor 41.

  When there is no x-axis rotation, the coordinates of the pixel that has detected the amount of light corresponding to the beam irradiation position coincide with the coordinates of the target value. In this case, the MEMS mirror 24 is assembled to the housing without a rolling error. On the other hand, if there is x-axis rotation, a deviation occurs between the beam irradiation position and the target value. As shown in FIG. 7, the deviation from the target value is the sum of the scanning position deviation and the writing position deviation at the center of the image height, and the larger the deviation amount R3, the larger the x-axis rotation amount. If the deviation amount R3 is obtained, the x-axis rotation amount of the MEMS mirror 24 can be obtained based on the graph of FIG. Then, based on the table in Table 1, the write timing correction amount corresponding to the shift amount R3 is corrected, and on the basis of the table 2, partial equality (scanning position shift) is corrected according to the shift amount R3. A quantity can be derived.

[Step 11]
Using the first and second jig BD sensors 33 and 34 (first and second optical sensors), the MEMS mirror 24 is swung around the swing shaft 24S, and the deflection angle of the MEMS mirror 24 is adjusted. Since the MEMS mirror 24 has individual variations, it is necessary to adjust the deflection angle by individually adjusting the driving conditions. The deflection angle adjustment, the deflection angle θ of the MEMS mirror 24, it is to regulate the maximum deflection angle A ₁ shown in the supra formula (2), the driving condition so as to satisfy the lens characteristics. Further, when the x-axis rotation is present in the MEMS mirror 24, the driving condition must be adjusted in consideration of the x-axis rotation amount.

First, the adjustment when no x-axis rotation occurs is an adjustment that eliminates only the individual variation. As described above, the image height at which the first and second jig BD sensors 33 and 34 are installed is known. Further, since _{A 1} of formula (2) is a fixed value, first when the MEMS mirror 24 is swung, the second jig BD sensor 33 and sequentially detects the deflected light beam L2 a BD signal output The time interval tij (i, j = 1, or 2) to be determined is naturally determined. Here, “i” and “j” indicate “first” and “second” of the jig BD sensors 33 and 34, and the arrangement of ij indicates the output order of the BD signals. For example, “t12” indicates a time interval from when the first jig BD sensor 33 detects the deflected light beam L2 to when the second jig BD sensor 34 detects the deflected light beam L2. “T22” indicates a time interval from when the deflected light beam L2 scans on the second jig BD sensor 34 to the time when the swing direction is reversed and then the second jig BD sensor 34 is scanned again.

In this case, the driving condition of the MEMS mirror 24 is adjusted so that the time interval tij shown in the following Table 3 is obtained. As shown in Table 3, since it is assumed here that no x-axis rotation has occurred, A ₀ = 0 in equation (1).

On the other hand, when the x-axis rotation occurs, that is, when A ₀ ≠ 0, the time interval tij of the BD signal corresponding to A ₁ is different as can be seen from the equation (1). It is necessary to correct this. FIG. 11 shows fluctuations in the time intervals t21 and t11 accompanying the x-axis rotation. Further, FIG. 12 shows the fluctuation of the time intervals t12 and t22 accompanying the x-axis rotation. In addition, t12 and t21 show the same fluctuation. Any time interval tij changes linearly according to the x-axis rotation amount.

  Table 4 is a table showing correction values for the time interval tij of the BD signal. If the x-axis rotation amount of the MEMS mirror 24 is obtained in step 10, the time interval tij is corrected according to the x-axis rotation amount with reference to the following Table 4. Then, the driving condition of the MEMS mirror 24 is adjusted based on the corrected time interval tij.

[Step 12]
The first BD sensor 31 and the second BD sensor 32 are fixed at predetermined positions of the housing of the optical scanning device 11.

[Step 13]
The time during which the MEMS mirror 24 is swung around the swing shaft 24S with the drive parameters obtained in the above step 11, and the first and second BD sensors 31, 32 sequentially detect the deflected light beam L2 and output the BD signal. The interval tij (i, j = 3, 4) is measured. Here, “3” and “4” indicate “first BD sensor 31” and “second BD sensor 32”, respectively. Since known driving parameters are used, position information of the first BD sensor 31 and the second BD sensor 32 can be acquired based on the measured time interval tij.

The time interval tij (i, j = 3, 4) obtained based on the BD signals of the first and second BD sensors 31 and 32 corrects the driving condition of the MEMS mirror 24 after the optical scanning device 11 is assembled. It can be used as a reference value when That, MEMS mirrors 24, be given a certain driving conditions, the operating environment of the optical scanning device 11 (temperature, humidity, atmospheric pressure, etc.) the parameters _{A 1} through changes. Accordingly, it is necessary to readjust the driving conditions of the MEMS mirror 24 after the assembly of the optical scanning device 11 is completed and mounted in the main body of the image forming apparatus 1. For this readjustment, the first and second BD sensors 31 and 32 are used. The time interval tij (i, j = 3, 4) obtained in step 13 is used as a reference, and the MEMS mirror 24 is adjusted. The driving conditions are adjusted.

[Step 14]
The x-axis rotation amount of the MEMS mirror 24, the light amount of the semiconductor laser 21, the driving conditions of the MEMS mirror 24, the position information of the first and second BD sensors 31, 32, etc. obtained in the above steps are stored in a predetermined storage device (for example, And stored in a storage unit 62) shown in FIG. By performing steps 1 to 14 as described above, it is not necessary to perform x-axis rotation adjustment, and it is not necessary to perform a special step for measuring the x-axis rotation amount. Therefore, the assembly process of the optical scanning device 11 can be simplified.

  Next, the electrical configuration of the image forming apparatus 1 will be described. FIG. 13 is a block diagram illustrating an electrical configuration of the image forming apparatus 1. The image forming apparatus 1 includes a control unit 60 (a part of the control unit) that comprehensively controls the operation of each unit of the image forming apparatus 1. The control unit 60 includes a CPU (Central Processing Unit), a ROM (Read Only Memory) that stores a control program, a RAM (Random Access Memory) that is used as a work area of the CPU, and the like. The image forming apparatus 1 includes an image forming unit 63, an operation unit 64, an image memory 65, and an I / F (interface) 66 in addition to the optical scanning device 11 and the fixing device 16 described above.

  The image forming unit 63 performs an image forming process on the recording paper, and includes the developing device 12, the charger 13, the photosensitive drum 14, the transfer roller 15, and the like. The operation unit 64 includes a liquid crystal touch panel, a numeric keypad, a start key, a setting key, and the like, and receives user operations and various settings for the image forming apparatus 1.

  The image memory 65 temporarily stores image data for printing given from an external device such as a personal computer. The I / F 66 is an interface circuit for realizing data communication with an external device. For example, the I / F 66 creates a communication signal according to a communication protocol of a network connecting the image forming apparatus 1 and the external device, and from the network side. Are converted into data in a format that can be processed by the image forming apparatus 1. A print instruction signal transmitted from a personal computer or the like is given to the control unit 60 via the I / F 66, and image data is stored in the image memory 65 via the I / F 66.

  The optical scanning device 11 includes an LD driving unit 21D (a part of the control unit), a MEMS driving unit 24D (driving unit), and the first and second BD sensors 31 and 32 described above. The LD driving unit 21D is a driver for driving the semiconductor laser 21, and controls the light emission timing of the semiconductor laser 21 by turning on the semiconductor laser 21 in accordance with a timing signal given based on the image data in the image memory 65.

  The MEMS driving unit 24D drives the MEMS mirror 24 by a so-called superposition driving method, and applies a sine wave voltage of a predetermined frequency to a coil provided in the mirror unit 241 so that the mirror unit 241 is pivoted. Reciprocate around the 24S axis. As a result, a deflected light beam L2 that can be deflected and scanned in the scanning region can be produced.

  The control unit 60 controls each unit of the image forming apparatus 1 by the CPU executing a control program stored in the ROM, and controls an image forming operation by the image forming apparatus 1. In the present embodiment, in particular, the control unit 60 includes an exposure control unit 61 and a storage unit 62 (storage means).

  The exposure control unit 61 controls the operation of the optical scanning device 11. For this control, the exposure control unit 61 gives the LD drive unit 21D a control signal for the light emission timing and light quantity of the semiconductor laser 21, and gives the MEMS drive unit 24D a control signal for the oscillation drive of the MEMS mirror 24. As a result, a predetermined amount of light beam is emitted from the semiconductor laser 21 at a predetermined writing timing, the light beam is reflected by the MEMS mirror 24 at a predetermined deflection angle, and the above-described deflected light beam L2 is produced.

  In the present embodiment, the exposure control unit 61 particularly includes a writing timing control unit 611 and a partial equality correction control unit 612. The writing timing control unit 611 refers to the storage unit 62 and corrects the timing (first timing) at which writing is started by laser light for one scanning line in accordance with the x-axis rotation amount described in detail above (Table 1). 1), the light emission timing of the semiconductor laser 21 is controlled. The partial equality correction control unit 612 similarly refers to the storage unit 62 and corrects the timing (second timing) at which each scanning position on one scanning line is irradiated with laser light according to the x-axis rotation amount. (See Table 2) The light emission timing of the semiconductor laser 21 is controlled so that it can be performed. In addition, the exposure control unit 61 refers to the outputs of the first and second BD sensors 31 and 32 in order to obtain the synchronization timing, and also refers to the storage unit 62 to correct the correction value (Table) of the time interval tij of the BD signal. 4), the driving condition of the MEMS mirror 24 is adjusted. By these correction controls, the x-axis rotation is canceled out, and the deviation of the writing timing and the scanning position is corrected.

  The storage unit 62 stores data on the x-axis rotation amount (rotation shift amount at the center of the deflection angle of the MEMS mirror 24 with respect to the optical axis of the imaging optical system) obtained in step 10 above, and the semiconductor laser 21 obtained in step 9. Data, the correction value according to the x-axis rotation amount of the writing timing, the correction value according to the x-axis rotation amount of partial equal magnification, the driving condition of the MEMS mirror 24 obtained in step 13 and the x A correction value or the like corresponding to the amount of shaft rotation is stored.

  Since the control unit 60 has the above-described configuration, the MEMS mirror 24 performs the photosensitive member in a state substantially equivalent to the x-axis rotation adjustment without performing the x-axis rotation adjustment when the optical scanning device 11 is assembled. The peripheral surface 14a of the drum 14 can be accurately deflected and scanned.

  According to the optical scanning device 11 according to the present embodiment described above, since the x-axis rotation adjustment process of the swing shaft 24S of the MEMS mirror 24 can be omitted, the manufacturing process can be simplified, and thus the light The manufacturing cost of the scanning device 11 can be suppressed. Further, since it is not necessary to provide the optical scanning device 11 with an x-axis rotation adjusting mechanism, the optical scanning device 11 can be downsized.

DESCRIPTION OF SYMBOLS 1 Image forming apparatus 11 Optical scanning apparatus 14 Photosensitive drum (image carrier)
14a Circumferential surface (scanned surface)
21 Semiconductor laser (light source)
21D LD drive unit (part of control means)
22 Collimator lens 23 Cylindrical lens 24 MEMS mirror (deflector)
24S oscillating shaft 24D MEMS drive unit (drive means)
241 Mirror unit 242 Torsion bar 25, 26 First and second scanning lenses (imaging optical system)
31 First BD sensor (first optical sensor)
32 Second BD sensor (second optical sensor)
33 First jig BD sensor 34 Second jig BD sensor 51 Holding plate 52 Pressing protrusion (holding mechanism)
60 control unit 61 exposure control unit (part of control means)
62 Storage section (storage means)

Claims (6)

A light source that emits a luminous flux;
Control means for controlling the light emission timing of the light source;
A deflecting body having a rocking shaft, which reflects and scans a light beam emitted from the light source while swinging a sine with a predetermined swing angle around the shaft of the rocking shaft;
Drive means for driving the deflector;
An imaging optical system having an optical axis and imaging the light beam deflected and scanned on a scanned surface;
Storage means for storing the amount of rotational deviation of the center of the deflection angle of the deflecting body with respect to the optical axis of the imaging optical system,
The control means has a first timing for starting irradiation of the light beam on the surface to be scanned for one main scanning line, and a second timing for performing irradiation of the light beam on each scanning position on the main scanning line. Is corrected in accordance with the amount of rotational deviation, and the light emission timing is controlled. The optical scanning device according to claim 1,
The deflector is
A mirror part for reflecting the luminous flux;
A torsion bar disposed on the rocking shaft and supporting the mirror part,
The driving means includes
An optical scanning device that swings the mirror portion with a predetermined sine wave. The optical scanning device according to claim 2, further comprising:
A first rotation adjusting mechanism that rotates the deflecting body around the axis of the first axis along the normal line of the mirror unit, and adjusts the rotational position of the deflecting body around the axis of the first axis;
A second rotation adjusting mechanism for rotating the deflecting body about an axis of a second axis orthogonal to the first axis and the swinging axis and adjusting a rotational position of the deflecting body about the axis of the second axis; An optical scanning device. The optical scanning device according to claim 3, further comprising:
An optical scanning device comprising a holding mechanism that prohibits the mirror portion from swinging about the swing shaft when the rotational position is adjusted by the first rotation adjustment mechanism and the second rotation adjustment mechanism. . The optical scanning device according to claim 1, further comprising:
A first optical sensor disposed on a scanning start side of the main scanning line and detecting a light beam emitted from the light source;
A second optical sensor disposed on the scanning end side of the main scanning line and detecting a light beam emitted from the light source,
The driving means includes
The deflecting body is driven based on a parameter that depends on a time interval of a timing at which the first light sensor and the second light sensor sequentially detect the light flux,
An optical scanning device that corrects the time interval according to the amount of rotational deviation and drives the deflector based on a correction parameter derived according to the corrected time interval. An image carrier for carrying an electrostatic latent image;
The optical scanning device according to any one of claims 1 to 5, which irradiates a light beam with the peripheral surface of the image carrier as the surface to be scanned.
An image forming apparatus comprising:

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