JP5219400B2 - Optical scanning device - Google Patents

Description

  The present invention relates to an optical scanning device that scans an image carrier by deflecting laser light from a light source.

  Conventionally, as a method for attaching an imaging lens for imaging a laser beam on an image carrier to an optical box in an optical scanning device, there is a method described in Patent Document 1.

  As shown in FIG. 7, in Patent Document 1, the plastic lens 3 includes a lens portion 301 and a short-side rib 302 and a long-side rib 303 formed so as to surround the lens portion 301. The long-side rib 303 is provided with a protrusion 304 at the center position in the lens scanning direction (arrow X in the figure) on the side in contact with the positioning reference surface 601 for the housing 6. The projection 304 is fitted and engaged with the recess 602 of the housing 6 to perform positioning in the scanning direction. Thereby, the thermal expansion of the plastic lens 3 can be released to both ends with the center in the scanning direction X as a reference.

JP 07-199100 A

  However, the optical scanning device described in Patent Document 1 has the following problems.

  In the optical scanning device when the scanner motor is driven, a temperature rise in the optical scanning device due to heat generated from the scanner motor and an air flow due to rotation of the rotary polygon mirror occur, resulting in an uneven temperature distribution. In particular, the imaging lens arranged in the vicinity of the scanner motor is likely to receive heat from the scanner motor, and is susceptible to air flow due to rotation of the rotary polygon mirror.

  The air on the imaging lens surface flows from the image writing start side to the image writing end side on the imaging lens surface. As a result, the temperature at the image writing start side in the scanning direction of the imaging lens closest to the scanner motor is higher than the temperature at the image writing end side.

  FIG. 8 is a table showing the results of measuring the imaging lens surface temperature when the scanner motor is continuously driven. As shown in FIG. 8, when the scanner motor is continuously driven, the temperature of the imaging lens surface is about 2 ° C. at the image writing start side (about 42 ° C.) and the image writing end side (about 40 ° C.). There is a difference.

  When the temperature on the image writing start side becomes higher, the refractive index on the left side of the imaging lens is further changed to generate a “single magnification difference” that causes a difference in the magnification of the left and right images with respect to the image center. In particular, in Patent Document 1, the positioning of the imaging lens with respect to the optical box is based on the vicinity of the center in the deflection scanning direction. For this reason, the left and right refractive indexes change asymmetrically to generate a “single magnification difference” that causes a difference in the magnification of the left and right images with respect to the image center, thereby degrading the image quality.

  Particularly in recent years, the amount of heat generated has increased with the increase in the speed of the scanner motor of the deflecting means, and the imaging lens has been provided close to the scanner motor, which is a heating element, due to the downsizing of the optical scanning device. It is easy to be affected.

  The present invention reduces the left-right image magnification difference with respect to the center of the image and reduces the “single-magnification difference” due to temperature rise, even when a non-uniform temperature distribution occurs on the left and right of the imaging lens by driving the scanner motor. An object of the present invention is to provide an optical scanning device capable of improving image quality.

Typical configuration of an optical scanning apparatus according to the present invention in order to solve the above problems, a light source for emitting a laser beam, a deflecting means for deflecting the laser beam emitted from the light source, deflected by the deflecting means laser light passes through a lens causes imaging the laser beam on the image bearing member, anda housing for supporting the lens, the laser beam deflected by said deflecting means, said of the lens In the optical scanning device that performs scanning with the laser beam on the image carrier by transmitting the lens while moving from one end to the other end in the scanning direction on the scanning region corresponding to the image region of the image carrier , lens, the position of the scanning direction against the housing includes a is fixed positioning portion, the temperature of the lens by the temperature rise in the apparatus is higher than it is the other end of the one end of the scanning region, Serial positioning unit, with respect to the scanning direction, characterized in that it only provided on the one end side than the center of the scanning area of the lenses.

  According to the present invention, even when a non-uniform temperature distribution occurs on the left and right of the imaging lens by driving the scanner motor, the left and right image magnification difference with respect to the center of the image is reduced, and the “single magnification difference” due to temperature rise is reduced. Can be reduced and the image quality can be improved.

(First embodiment)
Exemplary embodiments of the present invention will be described in detail below with reference to the drawings. However, the dimensions, materials, shapes, relative arrangements, and the like of the components described in this embodiment are not intended to limit the scope of the present invention only to those unless otherwise specified. Absent.

(Optical scanning device)
FIG. 1 is a configuration diagram of an optical scanning device according to the present embodiment. As shown in FIG. 1, the optical scanning device includes an optical box 10, a semiconductor laser device 1, a collimator lens 1a, a cylindrical lens 2, a rotary polygon mirror 3, a scanner motor 3b, and imaging lenses 4a and 4b.

  The optical box 10 accommodates various optical members. A light beam emitted from the semiconductor laser device 1 serving as a light source is converted into a parallel light beam by the collimator lens 1 a and condensed linearly by the cylindrical lens 2.

  The rotary polygon mirror 3 is a deflecting means having a deflecting reflecting surface in the vicinity of a line image of a light beam formed by being condensed by the cylindrical lens 2. The scanner motor 3 b is means for rotating the rotary polygon mirror 3. The light beam deflected and reflected by the rotary polygon mirror 3 irradiates a photosensitive member (not shown) as an image carrier through the imaging lenses 4a and 4b.

  The imaging lenses 4a and 4b are designed so that the light beam reflected by the rotary polygon mirror 3 is condensed so as to form a spot on the photosensitive member, and the scanning speed of the spot is kept constant. . As the rotary polygon mirror 3 rotates, the photoconductor performs main scanning with a light beam, and the photoconductor rotates and rotates around the axis of the cylinder. In this way, an electrostatic latent image is formed on the surface of the photoreceptor.

The imaging lens 4a arranged at the closest distance to the scanner motor 3b has a convex functioning as a positioning unit for the optical box 10 at a position shifted from the center L of the image area in the scanning direction of the laser light toward the image writing start side. Part 11 is provided. On the other hand, the optical box 10 is provided with a concave portion 12 facing the convex portion 11. The imaging lens 4 a is disposed at a predetermined position of the optical box 10 by the convex portion 11 and the concave portion 12. That is, the convex portion 11 and the concave portion 12 are fitted, and the side surface of the convex portion 11 abuts on the reference surface of the concave portion 12, whereby the imaging lens 4a is positioned in the optical box 10 in a direction substantially parallel to the scanning direction. The

(Image forming device)
An image forming technique using a photoconductor is well known as an electrophotographic recording technique, and therefore will not be described in detail and will be described briefly.

  A corona discharger that uniformly charges the surface of the photoconductor around the photoconductor, and a developing device (developing device) for developing the electrostatic latent image formed on the surface of the photoconductor into a toner image ), A transfer corona discharger (not shown) for transferring the toner image onto the recording paper is disposed. By these functions, recording information corresponding to the light beam generated by the semiconductor laser device is printed on the recording paper.

(Air flow inside the optical scanner)
The flow of air inside the optical scanning device will be described with reference to FIG. When the scanner motor 3b serving as a heat source of the optical scanning device rotates at a high speed, a warm air flow is generated inside the optical scanning device.

  As shown in FIG. 2, when the scanner motor 3b having the rotating polygon mirror 3 rotates at high speed in the rotation direction R, air flows from the rotating polygon mirror 3 toward the imaging lens 4a (in the direction of arrow B). Then, the air whose temperature has increased in the vicinity of the scanner motor 3b flows toward the writing start side in the scanning direction of the imaging lens 4a, and the temperature on the image writing start side becomes higher than the temperature on the image writing end side.

(Single magnification difference)
A change in the refractive index of the imaging lens caused by a non-uniform temperature distribution, a change in thermal expansion, and the accompanying “half magnification difference” on the left and right of the image area will be described using a comparative example.

  FIG. 3 is a diagram for explaining the variation of the scanning line in the comparative example. The imaging lens 4a receives heat from the scanner motor 3 and rises in temperature, and the image writing start side rises more than the image writing end side.

  As shown in FIG. 3, the regular scanning line L1 on the image writing start side is a scanning line when the rotary polygon mirror 3 is rotated to a state indicated by 3L1 before the temperature of the imaging lens 4a rises. Further, the regular scanning line L2 on the image writing end side is a scanning line when the rotary polygon mirror 3 is rotated to a state indicated by 3L2 before the imaging lens 4a rises in temperature.

  The regular scanning line L1 and the regular scanning line L2 change in the outward direction (arrow A1 direction, arrow A2 direction) as the imaging lens 4a undergoes thermal expansion change due to temperature rise. Here, since the temperature of the image writing start side is higher than that of the image writing end side, the fluctuation amount of the scanning line in the scanning direction is a1> a2. a1: Variation amount on the start side of image writing, a2: Variation amount on the end side of image writing. This is a “single magnification difference” that causes a difference in the magnification of the left and right images with respect to the image center L. The magnification difference (single magnification difference) Δa is Δa = a1−a2. The occurrence of this “single magnification difference” deteriorates the image quality.

  FIG. 4 is a diagram for explaining the variation of the scanning line in the present embodiment. As shown in FIG. 4, the positioning part (convex part 11) of the imaging lens 4a is shifted in parallel in the scanning direction by c from the center of the imaging lens 4a to the image writing start side. Due to the influence of air whose temperature has risen in the vicinity of the scanner motor 3b, the imaging lens 4a has an image writing start side of the imaging lens 4a in the direction of the arrow E1 with the positioning portion (convex portion 11) as the center. The image writing end side thermally expands in the direction of arrow E2. At this time, the length of the imaging lens 4a in the scanning direction is set so that the image writing end side is longer than the image writing start side with respect to the positioning portion, so that the thermal expansion amount of the imaging lens 4a is e2>. e1. e1: thermal expansion amount on the image writing start side of the imaging lens, e2: thermal expansion amount on the image writing end side of the imaging lens. That is, the center of the imaging lens 4a changes toward the end of image writing.

  Similar to the comparative example shown in FIG. 3, the imaging lens 4a thermally expands due to the temperature rise, so that the normal scanning line L1 and the normal scanning line L2 change in the outward direction (arrow A1 direction, arrow A2 direction). It is. However, the shift amount of the scanning line in the scanning direction is changed by the parallel shift of the positioning portion (convex portion 11) of the imaging lens 4a toward the image writing start side by c, so that the center of the imaging lens 4a changes toward the image writing end side. 3 is different from the comparative example shown in FIG.

  Here, the difference between the left and right magnifications (single magnification difference) Δb with respect to the image center L can be expressed as Δb = b1−b2. b1: Variation amount on the scanning line image writing start side, b2: Variation amount on the scanning line image writing end side.

  In the present embodiment, the center of the imaging lens 4a is shifted toward the end of image writing by shifting the positioning portion (convex portion 11) of the imaging lens 4a by c toward the image writing start side. The magnification difference (single magnification difference) Δa can be canceled out. That is, the amount c of shifting the positioning portion (convex portion 11) of the imaging lens 4a toward the image writing start side may be determined so that the magnification difference Δb = b1−b2 is as close to 0 as possible. By doing in this way, generation | occurrence | production of the difference (DELTA) b of the magnification by the nonuniform temperature rise which generate | occur | produced in the imaging lens 4a can be reduced.

(Example)
FIG. 5 is a diagram illustrating an appropriate arrangement of the positioning portion (convex portion 11) in the optical scanning device according to the present embodiment.

  In this optical scanning device, when the scanner motor is driven, the surface temperature of the imaging lens 4a increases by 10 ° C., and a temperature difference of 2 ° C. between the left and right in the scanning direction occurs.

An irradiation position deviation amount dY1 in the scanning direction generated by the change in the refractive index of the imaging lens 4a is dY1 = dy × Δn × ΔT = + 42.857 × 8.50 × 10 ⁻⁵ × 2≈ + 7.286 [μm]. Become. dy: Irradiation position shift sensitivity to change in refractive index: +42.857 [mm], Δn: Change in refractive index of imaging lens per unit temperature: 8.50 × 10 ⁻⁵ , ΔT: Temperature difference between right and left of imaging lens : 2 [° C.].

  The irradiation position shift amount dY1 = 7.286 [μm] generated by the refractive index change of the imaging lens 4a corresponds to a “single magnification difference” which is a magnification difference between the left and right images. This can be offset by an irradiation position shift caused by thermal expansion of the imaging lens 4a.

The irradiation position shift amount dY2 generated by the thermal expansion of the imaging lens 4a that cancels the irradiation position shift amount dY1 is dY2 = dY1 × Δy = 7.286 × 10 ⁻³ × (−0.8) = − 5.829. [Μm]. Δy: Irradiation position shift sensitivity to a single magnification difference: −0.8 [mm]).

  In order to set the irradiation position shift amount due to thermal expansion of the imaging lens 4a to −5.829 [μm], the positioning portion (convex portion 11) is written from the center L of the image area in the scanning direction of the imaging lens 4a. It may be provided by shifting dY3 toward the start side.

The distance dY3 from the center of the image area after the imaging lens 4a is thermally expanded to the positioning portion (convex portion 11) is dY3 = dY2 / (Δl × Δt) = − 5.829 × 10 ⁻³ /(6.0 × 10 ⁻⁵ × 10) ≈9.7 [mm]. Δl: linear expansion coefficient of imaging lens material: 6.0 × 10 ⁻⁵ , Δt: imaging lens rising temperature: 10 [° C.]).

  Therefore, the imaging lens positioning part (convex part 11) may be provided so as to be shifted by about 10 mm toward the writing start side in the scanning direction. By so doing, it is possible to efficiently offset the irradiation position deviation caused by the change in the refractive index of the imaging lens 4a and the irradiation position deviation caused by the thermal expansion change of the imaging lens 4a.

  The above numerical values are values specific to the imaging lens used in the verification experiment of the present invention, and change depending on the shape and optical characteristics of the imaging lens used in the optical scanning device. However, there is no change in the application in which the imaging lens is used, and the above numerical values do not deviate greatly in other imaging lenses.

  Moreover, although the present Example demonstrated the structure which used the positioning part of the imaging lens 4a as the convex part 11, and set the attachment part of the optical box 10 as the recessed part 12, this invention is not limited to this. For example, the same effect can be obtained even if the positioning portion of the imaging lens 4a is a concave portion and the mounting portion of the optical box 10 is a convex portion.

(Second Embodiment)
Next, a second embodiment of the optical scanning device according to the present invention will be described with reference to the drawings. FIG. 6 is an enlarged view of the vicinity of the positioning portion of the imaging lens in the optical scanning device according to the second embodiment. About the part which overlaps with said 1st embodiment, the same code | symbol is attached | subjected and description is abbreviate | omitted.

  As shown in FIG. 6, the optical scanning device of the present embodiment is configured by configuring the mounting portion 10b of the optical scanning device of the first embodiment with a pair of ribs 10c and 10d.

  The pair of ribs 10c and 10d are formed integrally with the optical box 10 and are opposed to each other. Of the pair of ribs, the positioning rib 10d is formed so as to be hardly deformed, and the other rib 10c is configured to be elastically deformable.

  The convex portion 11 that is a positioning portion of the imaging lens 4a is inserted between the pair of ribs 10c and 10d. The imaging lens 4a is attached to the optical box 10 by pressing and pressing the convex portion 11 against the other rib 10d by the elastic restoring force C of the rib 10c.

  With this configuration, the imaging lens 4a can be accurately positioned on the optical box 10 regardless of the dimensional variations of the mounting portion 10b of the optical box 10 and the convex portion 11 of the imaging lens 4a.

  By applying the optical scanning device according to the first and second embodiments to an image forming apparatus such as a printer, a facsimile machine, or a copying machine, the exposure scanning accuracy when performing exposure scanning on the image carrier is improved. It also leads to an improvement in the quality of the image to be formed. In particular, the effect is great in the case of an apparatus that forms a color image by superimposing a plurality of images.

1 is a configuration diagram of an optical scanning device according to a first embodiment. FIG. FIG. 3 is a diagram illustrating the air flow inside the optical scanning device according to the first embodiment. It is a figure explaining the fluctuation | variation of the scanning line in a comparative example. FIG. 6 is a diagram for explaining the variation of the scanning line in the first embodiment. FIG. 5 is a diagram illustrating an appropriate arrangement of positioning portions in the optical scanning device according to the first embodiment. It is an enlarged view near the positioning part of the imaging lens which concerns on 2nd Embodiment. It is a block diagram of the conventional optical scanning device. It is a figure which shows the imaging lens surface temperature measurement result at the time of the conventional scanner motor continuous drive.

Explanation of symbols

1 ... Semiconductor laser device (light source)
10: Optical box 11: Convex part (positioning part)
3 ... rotating polygon mirror 4 ... imaging lens

Claims (4)

A light source for emitting a laser beam, a deflecting means for deflecting the laser beam emitted from said light source, said deflection unit laser beam deflected is transmitted by the lens causes imaging the laser beam on the image bearing member has a housing for supporting the lens, the laser beam deflected by the deflecting means, to the other end of the scanning region above the one end in the scanning direction corresponding to the image region of said image bearing member in the lens In an optical scanning device that performs scanning with a laser beam on the image carrier by transmitting through the lens while moving,
The lens is provided with a positioning portion which was decided position in the scanning direction against the housing,
Due to the temperature rise in the apparatus, the temperature of the lens becomes higher at one end side of the scanning region than at the other end side, and the positioning portion is on the one end side from the center of the scanning region of the lens in the scanning direction. The optical scanning device is provided only in the above. The optical scanning device according to claim 1, wherein the positioning unit is provided between both ends of a scanning region of the lens in the scanning direction. The said deflection | deviation means is provided with the rotary polygon mirror and the motor which rotates the said rotary polygon mirror, The one end of the said scanning area | region is in the said scanning direction upstream rather than the other end, The Claim 1 or 2 characterized by the above-mentioned. Optical scanning device. Wherein the housing includes a fixing portion for positioning and fixing the positioning unit,
The fixing portion is a pair of ribs facing each other in the scanning direction, and at least one of the pair of ribs is elastically deformable, and is elastically deformed between the pair of ribs in the scanning direction by an elastic restoring force of the ribs. the optical scanning apparatus according to any one of claims 1 to 3, characterized in that sandwich the positioning portion.

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