JP2001330790A - Optical scanning optical device and image forming device using the same - Google Patents

Abstract

PROBLEM TO BE SOLVED: To obtain an optical scanning optical device which can effectively lessen the flare light generated by the incident of luminous fluxes on a flange part disposed at the end in the main scanning direction of a long-sized plastic lens and an image forming device using the same. SOLUTION: This optical scanning optical device has a light source means 2, a first optical system 42 which makes the luminous fluxes emitted from this light source means incident on a deflecting means 10 and a second optical system 43 which images the luminous fluxes deflected and reflected by the deflecting means to the effective scanning region on a surface 12 to be scanned. The second optical system has >=1 plastic lens. This plastic lens has the flange part 54 for reinforcement at the end in the main scanning direction and the region corresponding to the incident surface and/or or exit surface of the lens through which the luminous fluxes incident on the flange part are transmitted is formed in a non-mirror surface (for example, diffusion surface).

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical scanning optical device and an image forming apparatus using the same, and more particularly, to a lens surface through which a light beam incident on a reinforcing flange provided at an end of a long plastic lens is transmitted. By forming the region as a non-mirror surface portion, generation of flare light is reduced, which is suitable for a device such as a digital copying machine or a laser printer.

[0002]

2. Description of the Related Art Conventionally, an optical scanning optical device has been widely applied as a writing optical system for a laser beam printer (LBP), a digital copying machine and the like. In recent years, with the spread of these devices, demands for higher image quality and higher speed are increasing. For example, in order to improve the image quality with a resolution of 600 dpi or more, it is necessary to form a minute spot of about 60 μm on the surface to be scanned. However, since the diameter of the light beam to be scanned becomes large, it is necessary to enlarge the optical deflector (polygon mirror). Therefore, there is a problem that it is difficult to achieve compatibility with high speed.

However, various approaches for increasing the speed have been proposed. For example, a multi-beam scanning method in which the number of beams is increased to perform parallel line scanning, or a conventional UFS (Und
OFS (Over Filled Scann), which can make polygon mirrors smaller and more versatile than the ER Filled Scanner method (UFS optical system)
er) method (OFS optical system) has been proposed.

The OFS system is promising as a system that overcomes the problem of speeding up the UFS system described below.

The UFS system is a system in which a light beam having a predetermined width for forming a minute spot, which is narrower than the width of the deflecting surface in the main scanning direction, is incident on one deflecting surface (reflection surface) of the polygon mirror, and deflects and scans. is there. In this UFS method, the position of the incident light beam on the deflection surface changes with the rotation of the deflection surface.In order to prevent the incident light beam from being vignetted in a predetermined scanning angle range, the width of the deflection surface in the main scanning direction is reduced. There has been a problem that the size of the polygon mirror must be larger than a certain value, and the shape of the polygon mirror becomes large. Increasing the number of deflection surfaces of the polygon mirror
Furthermore, it is difficult to rotate at high speed because the shape becomes large and the rotational load increases. Therefore, the UFS method generally employs a method of increasing the speed by multi-beaming, and requires a complicated configuration for multi-beaming.

The ratio between the theoretical scanning angle that can be scanned by one deflection surface and the scanning angle that scans the effective scanning area is called scanning efficiency. In the UFS method, since the incident light beam has a predetermined light beam width,
The scanning angle is a constraint that the incident light beam is not vignetted on the deflection surface. UF with large beam diameter and high resolution specification
In the S system, the scanning efficiency is at most about 70%. The remaining 30% is allocated before and after the image forming area, and is used for electrical processing such as stabilizing a light source at a predetermined output and detecting timing of an image writing position.

The light source is turned off immediately after the scanning of the one-line image forming area is completed. This is because unnecessary light that does not contribute to scanning hits the end of the optical member or the structure that supports the optical member, and reflected light or scattered light reaches the surface to be scanned as flare, deteriorating the image. I'm preventing.

On the scanning start side, it is necessary to turn on the light source before the effective scanning area in order to detect the writing start position of the image. Therefore, the occurrence of the same flare is inevitable. By devising the shape of the member, even if flare light is generated, it does not reach the surface to be scanned.

On the other hand, in the OFS method, a light beam emitted from a light source is made incident on a deflecting surface of a polygon mirror in a state wider than the width of the deflecting surface in the main scanning direction (the luminous beam is incident on a plurality of deflecting surfaces of the polygon mirror). ), And 1
This is a method in which one deflection surface rotates and scans. Since the incident light beam width is set sufficiently large, there is no fear that the light beam is vignetted by the scanning angle of the polygon mirror. The width of the deflection surface is UF
Since the width of the incident light beam can be matched with that in the S method, the polygon mirror diameter does not increase as in the UFS method even if the number of deflection surfaces is increased, and high-speed scanning can be performed by increasing the number of surfaces.

The OFS method can perform scanning with a scanning efficiency of 100% in principle, but in reality, it detects the time for stabilizing the output of the light source and the timing of the image writing position until the start of scanning. To save time,
For example, the scanning efficiency can be suppressed to about 90%.

As described above, in the OFS method, the number of surfaces can be increased without increasing the size of the polygon mirror, and the scanning efficiency can be increased, so that the speed of the scanning optical device can be increased. Needless to say, further speedup can be expected if the OFS method is changed to multibeam.

As the speed of the apparatus increases, the scanning time for one line is shortened, and considerable high-speed processing is required within a short lighting preparation period before the start of scanning. These processing speeds have a limit determined by the performance of the circuit control device, the stability of the rise of the light source, and the like.

Further, since the scanning efficiency is higher in the OFS system than in the UFS system, the situation is more severe, and there is little time to temporarily turn off the light source immediately after the end of the effective scanning area of one line. In other words, if the light source is turned off once because the next line scanning starts immediately, a rising time until the light amount reaches a predetermined amount after the light source cannot be secured, and the image writing position detection performed before the start of the line scanning is detected. In addition, there is a problem in that the accuracy of detection of the output of the light source and the like deteriorates, leading to deterioration of the image, and an optical system that does not turn off the light flux is required.

[0014]

A plastic lens is often used for the scanning lens of the scanning optical system in order to improve the performance and reduce the cost. Since this plastic lens has a softer lens surface than a conventional glass lens and is easily damaged, a flange is projected on an outer peripheral portion to structurally protect the lens surface. If the lens is elongated in the main scanning direction due to the arrangement of the lenses, it is necessary to structurally reinforce the lens end, and a reinforcing flange is required on the side surface of the end in the main scanning direction. Since the reinforcing flange has an inclination in the optical axis direction in the main scanning section, when unnecessary scanning light enters, it is reflected by the inclined part of the flange and becomes flare light toward the image forming area.

Therefore, in a scanning optical system having high scanning efficiency, it is inevitable that scanning light is incident on the reinforcing flange.
Flare measures are required.

According to the present invention, a reinforcing flange is provided at an end of the at least one long plastic lens constituting the second optical system in the main scanning direction, and a lens through which a light beam incident on the flange is transmitted. An optical scanning optical device capable of effectively reducing flare light and an image forming apparatus using the same are provided by forming a corresponding area of the incident surface and / or the exit surface on a non-mirror surface (for example, a diffusion surface). Aim.

[0017]

According to the first aspect of the present invention, there is provided an optical scanning optical apparatus, comprising: a light source; a first optical system for causing a light beam emitted from the light source to enter a deflection unit; A second optical system that forms an image of the light beam deflected and reflected in the effective scanning area on the surface to be scanned, wherein the second optical system has one or more plastic lenses. The plastic lens has a reinforcing flange portion at an end in the main scanning direction, and a corresponding area of an entrance surface and / or an exit surface of the lens through which a light beam incident on the flange portion is formed is a non-mirror surface portion. It is characterized by:

A second aspect of the present invention is characterized in that, in the first aspect of the invention, the non-mirror surface is a diffusion surface.

According to a third aspect of the present invention, in the second aspect, the diffusion surface has a transmittance characteristic of 10% or less.

According to a fourth aspect of the present invention, in the first aspect of the present invention, the non-mirror surface is a surface having an optical attenuation function.

According to a fifth aspect of the present invention, in the first aspect of the present invention, the distance between the non-specular surface area and the principal ray of the light beam heading toward the end of the effective scanning area is the light beam width in the main scanning direction of the light beam. Or more than half the value of

According to a sixth aspect of the present invention, in the first aspect of the present invention, the angle formed between the flange portion and the principal ray of the light beam heading toward the center of the effective scanning area is determined by the incidence of the principal ray of the light beam incident on the flange portion. It is characterized in that it is larger than the angle.

According to a seventh aspect of the present invention, in the first aspect, the optical scanning optical device controls the timing of a scanning start position on the surface to be scanned by using at least a part of a light beam that scans outside the effective scanning area. The light source means is always lit even when the light beam scans outside the effective scanning area.

According to an eighth aspect of the present invention, in the first aspect, the light beam passing through the first optical system is obliquely incident on the deflecting surface of the deflecting means in the sub-scan section. Features.

According to a ninth aspect of the present invention, in the first aspect of the present invention, the light beam passing through the first optical system is incident on the deflection surface from within the deflection angle of the deflection means in the main scanning section. And

According to a tenth aspect of the present invention, there is provided an image forming apparatus comprising: the optical scanning optical device according to any one of the first to ninth aspects;
A photoconductor disposed on a surface to be scanned of the scanning optical device; a developing unit for developing an electrostatic latent image formed by scanning the photoconductor with a light beam as a toner image; and the developed toner image And a fixing unit for fixing the transferred toner image to the sheet.

According to an eleventh aspect of the present invention, in the tenth aspect, an image is formed by a BAE process.

According to a twelfth aspect of the present invention, there is provided an optical scanning optical device, comprising: a light source; and a light beam emitted from the light source being incident on a deflecting surface of the deflecting device in a state wider than the width of the deflecting surface in the main scanning direction. In an optical scanning optical apparatus comprising: a first optical system; and a second optical system that forms a light beam deflected and reflected by the deflecting means on an effective scanning area on a surface to be scanned, the second optical system includes: The plastic lens has at least one plastic lens, the plastic lens has a reinforcing flange at an end in the main scanning direction, and corresponds to an entrance surface and / or an exit surface of a lens through which a light beam incident on the flange is transmitted. The region is formed on a non-mirror surface.

According to a thirteenth aspect, in the twelfth aspect, the non-specular portion is a diffusion surface.

According to a fourteenth aspect, in the thirteenth aspect, the diffusing surface has a transmittance characteristic of 10% or less.

According to a fifteenth aspect of the present invention, in the twelfth aspect, the non-mirror surface is a surface having an optical attenuation function.

According to a sixteenth aspect of the present invention, in the twelfth aspect of the invention, the distance between the non-specular surface area and the principal ray of the light beam heading toward the end of the effective scanning area is the light beam width of the light beam in the main scanning direction. Or more than half the value of

According to a seventeenth aspect of the present invention, in the twelfth aspect, the angle formed between the flange portion and the principal ray of the light beam heading toward the center of the effective scanning area is equal to the incidence of the principal ray of the light beam incident on the flange portion. It is characterized in that it is larger than the angle.

According to an eighteenth aspect of the present invention, in the twelfth aspect, the optical scanning optical device controls a timing of a scanning start position on the surface to be scanned by using at least a part of a light beam that scans outside the effective scanning area. The light source means is always lit even when the light beam scans outside the effective scanning area.

According to a nineteenth aspect, in the twelfth aspect, the light beam passing through the first optical system is obliquely incident on the deflecting surface of the deflecting means in the sub-scan section. Features.

According to a twentieth aspect, in the twelfth aspect, the light beam passing through the first optical system is incident on the deflecting surface from within the deflection angle of the deflecting means in the main scanning section. And

According to a twenty-first aspect of the present invention, there is provided an image forming apparatus, comprising: the optical scanning optical device according to any one of the twelfth to twentieth aspects; a photosensitive member disposed on a surface to be scanned of the optical scanning device;
Developing means for developing, as a toner image, an electrostatic latent image formed by scanning a light beam on the photoreceptor; transfer means for transferring the developed toner image to paper; and transferring the transferred toner image to paper And fixing means for fixing the toner image to the image.

According to a twenty-second aspect, in the twenty-first aspect, an image is formed by a BAE process.

[0039]

[First Embodiment] FIG. 1A is a main scanning sectional view of a first embodiment of a scanning optical device of the present invention.
FIG. 1B is a cross-sectional view in the sub-scanning direction of FIG. 1A, and FIG. 1C is a cross-sectional view (AA 'cross-sectional view) of the main part of the incident optical system taken along a plane orthogonal to the main scanning cross-section.

In this specification, the main scanning section is a section of the scanning optical system projected on a plane perpendicular to the rotation axis of the polygon mirror, and the sub-scanning section is the same as the main scanning section passing through the rotation axis of the polygon mirror. A section cut by a plane perpendicular to the plane is called.

In the figure, reference numeral 1 denotes a laser unit (optical unit), which is formed by integrating a semiconductor laser (laser light source) 2 as light source means and a collimator lens unit 3 formed by bonding two spherical lenses. The collimator lens unit 3 is configured so as to perform predetermined optical adjustment.
A parallel light beam parallel to the optical axis is emitted. Further, the laser unit 1 is provided with a shift adjusting means (not shown) capable of being parallel-shifted and fixed by a predetermined amount in a direction indicated by an arrow E perpendicular to the optical axis of the collimator lens unit 3 in the main scanning section.

The semiconductor laser 2 according to the present embodiment is set not to be turned off even when the light beam scans outside the effective scanning area (ineffective scanning section), but to be always turned on. That is, the semiconductor laser 2 continues to be turned off even after the image formation is completed, and does not turn off until the next line scanning starts.

4 is a concave lens having a negative refractive power,
The parallel light beam emitted from the laser unit 1 is a weakly divergent light beam. Reference numeral 5 denotes an aperture stop, which regulates a passing light beam to form a beam shape. Reference numeral 6 denotes a cylindrical lens having a predetermined refractive power only in the sub-scanning direction. Reference numeral 7 denotes a return mirror that bends the optical path of the light beam that has passed through the cylindrical lens 6 toward the optical deflector 10.

Each element of the collimator lens section 3, concave lens 4, aperture stop 5, cylindrical lens 6, and return mirror 7 constitutes one element of the incident optical system 41. The first, which will be described later,
Lens elements 8 and 9 constitute one element of the first optical system 42.

Reference numeral 10 denotes a polygon mirror (optical deflector) as a deflecting means, which is a driving means such as a motor (not shown).
As a result, it is rotating at a constant speed in the direction of arrow P in the figure.

A second optical system 43 has an fθ lens system 44 having first and second fθ lenses and a long cylindrical lens (long cylindrical lens) 11 made of a plastic material. . Lens system 44 in the present embodiment has a spherical concave lens 8 as a first fθ lens and a cylindrical lens 9 as a second fθ lens, and has a refractive power mainly in the main scanning direction,
The fθ characteristic and the curvature of field in the main scanning direction are favorably corrected over the effective scanning area. Long cylindrical lens 1
Numeral 1 mainly has a refractive power in the sub-scanning direction, makes the deflecting surface of the polygon mirror 10 and the surface to be scanned substantially conjugate in the sub-scanning cross section, and serves as the surface to be scanned due to the inclination of the deflecting surface. Of the irradiation position on the photosensitive drum surface 12 and uneven image pitch are prevented. The long cylindrical lens 11 suppresses the curvature of field on the photosensitive drum surface 12 in the sub-scanning direction, and keeps the magnification substantially constant to suppress the fluctuation of the spot diameter.

The reason that the long cylindrical lens 11 is provided with a refractive power mainly in the sub-scanning direction and is disposed in the vicinity of the photosensitive drum surface 12 is as follows.
This is to reduce the occurrence of pitch unevenness with respect to the eccentricity around the rotation axis of the polygon mirror 10 by setting the image forming magnification in the sub-scanning direction to 1 or less.

Reference numeral 12 denotes a photosensitive drum surface as a surface to be scanned.

Reference numeral 13 denotes a light shielding member, which is a polygon mirror 1
0 and the fθ lens system 44, unnecessary light fluxes on the scanning start side and scanning end side deflected and reflected by the polygon mirror 10 (effective scanning area of the light flux deflected and reflected by the polygon mirror 10) At least a part of the light beam that scans outside is shielded.

Reference numeral 34 denotes a reflection mirror (hereinafter, also referred to as a “BD mirror”), which is arranged on a scanning line in the main scanning direction, and performs synchronous detection for adjusting the timing of the scanning start position on the photosensitive drum surface 12. (A BD light beam) is reflected toward a synchronization detecting element 38 described later. Reference numeral 36 denotes a synchronization detection slit (hereinafter, also referred to as a “BD slit”), which is disposed at a position equivalent to the photosensitive drum surface 12.
Determines the starting position of the image. Reference numeral 37 denotes a condensing lens (hereinafter also referred to as a “BD lens”) for making the BD mirror 34 and the synchronization detecting element 38 conjugate with each other, and corrects the tilt of the BD mirror 34. . 38
Denotes an optical sensor (hereinafter also referred to as a “BD sensor”) as a synchronization detecting element. In the present embodiment, a synchronization signal (B) obtained by detecting an output signal from the BD sensor 38 is indicated.
D signal) is used to adjust the timing of the scanning start position for recording an image on the photosensitive drum surface 12. The BD slit 36, the BD lens 37, and the BD sensor 38 constitute one element of the writing position detecting optical system 35.

In this embodiment, as described above, the light source is always turned on without being turned off even outside the effective scanning area in one line, thereby improving the detection accuracy of the image writing position and the output stability of the light source. And a good image is always obtained. Each element is set so that the scanning efficiency of the optical scanning optical device of the present embodiment is 80% or more.

Here, the optical function of this embodiment will be described with reference to FIG.

In FIG. 1A, a parallel light beam emitted from the laser unit 1 is converted into a weak divergent light beam by a concave lens 4, the light beam diameter is shaped by an aperture stop 5, transmitted through a cylindrical lens 6, and bent by a return mirror 7. Can be
This light beam forms the second and first f
transmitted through the .theta. lenses 9 and 8, and becomes a parallel light flux again and enters the deflection surface from substantially the center of the deflection angle of the polygon mirror 10 (front incidence). At this time, the light beam width of the parallel light beam is set to be sufficiently larger than the facet width of the deflection surface of the polygon mirror 10 in the main scanning direction. That is, a plurality of deflection surfaces of the polygon mirror 10 are irradiated (overfilled scanning system).

The light beam deflected and reflected by the polygon mirror 10 is shielded from unnecessary light beams on the scanning start side and the scanning end side by the light shielding plate 13, and the first and second fθ lenses 8,
9, the light is guided on the photosensitive drum surface 12, and the polygon mirror 10 is rotated in the direction of arrow P to scan the photosensitive drum surface 12 in the direction of arrow S with linear motion at a constant velocity. Thereby, the photosensitive drum surface 1 as a recording medium
2 is image-recorded.

At this time, a part of the light beam deflected and reflected by the polygon mirror 10 is reflected on the upstream side outside the effective scanning area.
The optical path is bent by the D mirror 34 and is incident on the write start position detecting optical system 35, and the write start position detecting optical system 3
At 5, the time when the light beam has passed is detected. That is, the light beam that has crossed the BD slit 36 is detected as a signal waveform by the BD sensor 38, and the rise time of the waveform is detected. By starting writing the image after a predetermined delay time from the time from the detection time to the start of writing the image, the writing start position between the lines can be aligned.

In this embodiment, the light beam emitted from the laser unit 1 is incident on the polygon mirror 10 from the scanning angle in the main scanning section via the first optical system 42 as described above, so that the polygon mirror 10 is deflected. The asymmetry due to the ingress and egress of the surface is reduced, thereby improving the imaging performance of the second optical system 43.

Next, the optical function of this embodiment will be described with reference to FIG.

In FIG. 1C, each optical element from the laser unit 1 to the cylindrical lens 6 is arranged on the same optical axis (AA '), and this optical axis AA' is a plane perpendicular to the rotation axis of the polygon mirror 10. (Line) inclined at an angle of θ / 2 with respect to BB ′. In the present embodiment, θ / 2 =
0.8 degrees. In the case of a configuration in which the oblique incidence angle θ / 2 is incident on the polygon mirror 10 from within the scanning range, the oblique incidence angle θ / 2 is indispensable for separating from the scanning light beam deflected and reflected by the polygon mirror 10. The oblique incident angle θ / 2 is preferably as large as possible for separation, but is preferably about 1 ° or less in order to suppress the imaging performance and the scanning line curvature without using a special lens.

The parallel light beam emitted from the laser unit 1 is converted into a weak divergent light beam by the concave lens 4, shaped into a predetermined light beam diameter by the aperture stop 5, and transmitted through the second and first fθ lenses 9 and 8 by the cylindrical lens 6. As a result, an image is formed on the deflection surface 10a of the polygon mirror 10. Folding mirror 7
Is arranged in parallel with the rotation axis of the polygon mirror 10, whereby the convergent light obliquely incident from the cylindrical lens 6 is not twisted, and the focal line incident on the deflection surface 10a is in a plane perpendicular to the optical axis. The orientation is maintained without rotation.

In the case of an optical system in which the light beam emitted from the light source is incident on the deflection surface of the optical deflector in the main scanning section, the position of the deflection surface of the optical deflector will be changed if the light source is always on. The rotation of the vessel may cause a vertical relationship with the incident light beam. In this case, the specularly reflected light from the deflecting surface returns to the light source, and a phenomenon occurs in which the output stability of the light source is significantly impaired.
It is meaningless if such a phenomenon occurs even if the light source is continuously turned on.

Therefore, in the present embodiment, as described above, the light beam passing through the first optical system 42 is obliquely incident on the deflecting surface 10a of the polygon mirror 10 in the sub-scanning cross section, so that the deflecting surface 10a Does not return to the light source, thereby obtaining further stability of the light source.

Further, in this embodiment, as described above, the angle of incidence of the light beam on the polygon mirror 10 in the main scanning section is reduced by making the light beam enter the deflection surface 10a of the polygon mirror 10 from an oblique direction. Can be made symmetrical with respect to the center of the image, and the asymmetry due to the entrance and exit of the deflecting surface of the polygon mirror 10 can be reduced to improve the imaging performance of the second optical system 43.

Next, the optical operation of this embodiment will be described with reference to FIG.

In FIG. 1B, a light beam incident on the deflecting surface 10a of the polygon mirror 10 from an oblique direction is deflected and reflected while drawing a conical surface as the deflecting surface 10a rotates. The optical axes of the first and second fθ lenses 8 and 9 are placed in a direction substantially parallel to the straight line BB ′ shown in FIG. I have. However, in practice, the first and second fθ lenses 8 and 9 are slightly inclined slightly less than 1 degree in the sub-scanning section with respect to this arrangement. Even if the light beam reflected by the return mirror 7 is specularly reflected on the surfaces of the first and second fθ lenses 8 and 9 by arranging it at such an inclination, the specularly reflected light is prevented from going to the surface to be scanned. be able to.

A long cylindrical lens 11 having a refractive power mainly in the sub-scanning direction is disposed between the second fθ lens 9 and the photosensitive drum surface 12 as described above. An image is formed in the sub-scanning direction, and the deflection surface 10a of the polygon mirror 10 and the photosensitive drum surface 12 are substantially conjugated to correct the surface tilt of the polygon mirror. In addition, the long cylindrical lens 11 has a curvature radius in the sub-scanning cross-section of the lens on both surfaces in order to suppress the field curvature in the sub-scanning direction on the photosensitive drum surface 12 and keep the magnification substantially constant to suppress the fluctuation of the spot diameter. It is changed in the longitudinal direction. Further, since the scanning trajectory of the light beam incident on the long cylindrical lens 11 is curved, the scanning line curve on the photosensitive drum surface 12 is suppressed, and the optical axis of the long cylindrical lens 11 is adjusted to improve the imaging performance. It is decentered in the sub-scanning direction, so that the incident light beam passes through a position off the optical axis.

FIG. 2 shows the lens shape of the eccentric long cylindrical lens 11. As shown in the figure, the light beam center is located above the lens optical axis. In order to realize such a lens shape, the long cylindrical lens 11 is formed by molding plastic. In addition, since the long cylindrical lens 11 does not need to have a refractive power in the main scanning direction, both surfaces have the same curvature, and have a shape having a constant thickness and stable moldability.

Table 1 shows the configuration of the optical system from the polygon mirror 10 to the photosensitive drum surface 12.

[0068]

[Table 1]

Next, the optical function of each optical element will be described.

The laser unit 1 adjusts the distance between the semiconductor laser 2 and the collimator lens unit 3 and the angle of view. The laser unit 1 emits a parallel light beam parallel to the optical axis of the collimator lens unit 3 and has a predetermined precision. Installed with. The collimator lens section 3 is composed of a bonded lens in which two spherical lenses different in glass material are concave and convex from the semiconductor laser 2 side to reduce the spherical aberration and the chromatic aberration. In the OFS optical system, a part of the parallel light beam emitted from the laser unit 1 is cut off by the deflecting surface 10a of the polygon mirror 10 in the main scanning direction to become a deflected light beam. Is shifted off-axis in proportion to, and the amount of spherical aberration included in the light beam increases. For this reason, a conventional UFS optical system requires a cemented lens that reduces spherical aberration in the OFS optical system even if the F value (F number) is sufficiently dark with a single lens. The chromatic aberration is performed for the purpose of suppressing the focus fluctuation because the wavelength of the semiconductor laser 2 changes at the environmental temperature.

The parallel light beam emitted from the laser unit 1 is converted by the concave lens 4 into a weakly divergent light beam, transmitted through the second and first fθ lenses 9 and 8, and converted again into an enlarged parallel light beam. With such an optical configuration, only the semiconductor laser 2 of the laser unit 1 and the collimator lens unit 3 are integrated and shifted in parallel in the main scanning direction, and the lateral shift of the laser intensity distribution in the parallel light beam due to the inclination of the chip of the semiconductor laser element. Can be corrected. FIG. 3C is a schematic diagram of a main part showing a correction state at this time. FIG. 3A shows a case where the chip of the semiconductor laser device is not tilted.
(B) shows a case where the chip of the semiconductor laser device is inclined.

The shift adjusting means is included in the configuration in the laser unit 1 and can shift in the main scanning direction while maintaining the positional relationship between the semiconductor laser 2 and the collimator lens unit 3 with respect to the member attached to the incident optical system 41. The mechanism is provided. The adjustment of the optical characteristics of the laser unit 1 performed on a single jig is performed by adjusting the focus and the angle of view, then shifting the light source 2 and the collimator lens unit 3 integrally in the main scanning direction, The shift amount is adjusted so that the ratio of the intensity of the light beam divided into two in the main scanning direction with respect to the light beam transmitted through the provided predetermined aperture is equal to or less than a predetermined value. The adjusted laser unit 1 has a laser intensity peak almost coincident with the optical axis of the incident optical system 41 and emits a parallel light beam parallel to the optical axis, so that compatibility as a single unit can be guaranteed.

The concave lens 4 is moved in the direction of the optical axis to correct the focus fluctuation in the main scanning direction. The purpose of correcting the focus in the main scanning direction is based on the following three reasons.

(1) In the OFS optical system, the width of the deflecting surface of the polygon mirror in the main scanning direction is smaller than that of the UFS optical system, and it is difficult to ensure equivalent surface accuracy in the main scanning direction.

(2) The luminous flux is divided into first and second fθ lenses 8,
9 is reciprocated, and the effect of the surface accuracy of the fθ lens is 2
Double. Further, in the OFS optical system, the number of polygon surfaces increases, so that the focal length of the fθ lens increases, and the sensitivity of the surface accuracy increases, so that focus fluctuation cannot be ignored.

(3) A mechanism for correcting the focus within a narrow range of the depth of focus is required for a demand for a high resolution and a minute spot.

On the other hand, the focus correction in the sub-scanning direction may be performed by adjusting the concave lens 4 and then moving the cylindrical lens 6 in the optical axis direction as before.

The folding mirror 7 is a folding mirror for causing the incident light beam to enter from the scanning center (substantially the center of the deflection angle) of the polygon mirror, and folds the first optical system 41 to make it compact. In addition, the return mirror 7 corrects an oblique incident angle error caused by a component tolerance of the incident optical system 41 from the laser unit 1 to the cylindrical lens 6.
In order to make the light enter the deflection surface 10a of the polygon mirror 10 at a predetermined angle, as shown in FIGS. 4 (A) and 4 (B), the initial position can be adjusted around the rotation axis parallel to the folding mirror 7 in the main scanning section. An adjustment mechanism is provided.

In FIGS. 4A and 4B, the axis of rotation substantially coincides with the height of the incident light beam, and the supporting members (7a, 7b) arranged at this height serve as fulcrums on the back surface of the mirror. The mirror is rotated and adjusted by turning the set screw shown. The folding mirror 7 is adjusted and fixed at a predetermined angle by observing the reflected light beam with an observation system (not shown).

The width of the light beam incident on the deflecting surface 10a of the polygon mirror 10 in the main scanning direction is limited by the aperture stop 5, and the deviation of the light beam due to the scanning angle of the polygon mirror 10, the tolerance of the incident optical system 41, and the deviation of the polygon mirror 10 In consideration of the positional accuracy, the width is set to about 2 to 3 times the width of the deflection surface 10a in the main scanning direction. In the present embodiment, the polygon mirror is a polygon mirror having a circumscribed circle diameter of 29 mm and 12 surfaces, and an incident light beam having a width of 7.5 mm and a width of approximately 18 mm. The width of the stop in the sub-scanning direction is related to the spot diameter on the photosensitive drum surface 12.

[Explanation of Operation of Light Shield] Next, the operation of the light shield 13 as a light shielding member will be described.

In the present embodiment, as described above, the semiconductor laser 2 is set not to be turned off but to be always turned on even when the light beam scans outside the effective scanning area (ineffective scanning section). Therefore, in the present embodiment, the unnecessary light beams on the scanning start side and the scanning end side among the light beams deflected and reflected by the polygon mirror 10 are blocked by the light shielding plate 13,
The first and second fθ lenses 8 and 9 and the long cylindrical lens 11 are irradiated outside the effective portion to prevent flare light from being generated.

In the present embodiment, the light shielding plate 13 is symbolically arranged between the polygon mirror 10 and the first fθ lens 8, but the invention is not limited to this. A plurality may be added before and after. As a result, the light shielding effect of the flare becomes more complete.

[Description of Shape of Boundary Portion of Deflection Surface] Next, the shape of the boundary portion (edge portion) of the adjacent surface (adjacent deflection surface) of the polygon mirror will be described with reference to FIGS. 5A and 5B. I do.

In this embodiment, the polygon mirror 10 is a regular polygon having 12 surfaces. A boundary portion (edge portion) 10b between adjacent surfaces of the polygon mirror 10 has a ridge-like edge shape, and has a certain width as shown in FIG. In the present embodiment, the width of the boundary portion 10b (the width in the direction in which the polygon mirror rotates) is equal to the light beam width W in the main scanning direction of the light beam deflected and reflected by the deflecting surface 10a of the polygon mirror 10, that is, with respect to the deflecting surface 10a. It is set to be 1% or less (preferably 0.02% to 1%). In the present embodiment, since the light source is constantly lit as described above, a moment occurs when the boundary 10b of the adjacent surface is directly opposed to the surface 12 to be scanned. At this time, a part of the light beam incident on the boundary 10b from the front is, as shown in FIG.
The light is specularly reflected at an intensity proportional to the width of b, and irradiates the center on the surface to be scanned 12 by following the same optical path as that of the ordinary scanning light to become flare light.

However, in this embodiment, as described above, the width of the boundary portion 10b is set to the scanning width W of the light beam reflected by the deflecting surface 10a of the polygon mirror 10 in the main scanning direction (that is, the deflecting surface 1).
0%), the flare light intensity ratio is also about 1%, which does not substantially affect the image. Further, in the present embodiment, the area where the intensity peak of the light beam in the main scanning direction is 90% or more is the boundary portion 10b of the adjacent surface of the polygon mirror.
It is set to be incident on.

As described above, in the present embodiment, in the optical scanning optical apparatus in which the light source is always turned on even outside the effective scanning area as described above, the width of the boundary 10b between the adjacent surfaces of the polygon mirror 10 is set to the deflecting surface of the polygon mirror 10. The polygon mirror 1 is set by setting it so as to be 1% or less with respect to the scanning width W of the light beam reflected by 10a in the main scanning direction.
Even if the reflected light from the zero boundary portion 10b reaches the surface to be scanned 12 as flare light, substantially no image deterioration occurs.

[Another Description of Shape of Boundary Part of Deflection Surface] FIG.
FIG. 2 is a schematic view of a main part of a main part of a polygon mirror. In the figure, at the boundary between adjacent surfaces of the polygon mirror 10, one deflecting surface extends to the other deflecting surface, and the length of the extending region 10c is equal to the length of the deflecting surface 10a of the polygon mirror 10. Light beam width W of light beam deflected and reflected in the main scanning direction
5% or less (preferably 1% to 5%). That is, the deflection surface 1 of the polygon mirror 10
0a is set such that one boundary portion extends from the adjacent surface and the other boundary portion extends to the adjacent surface.

As described above, in the present embodiment, by forming the shape of the boundary portion as described above, even if the incident light as shown in FIG.
Only the width of the deflecting surface 10a is increased by the light beam width γ of the extending deflecting surface.

In the case of the OFS optical system, the width of the deflecting surface in the main scanning direction determines the light beam width, that is, the spot diameter in the main scanning direction. Therefore, an allowable value may be determined so as to suppress the amount of change. Normally, a spot diameter of about 5% is permissible, and thus, by devising a processing method, when such an extended shape is formed, flare does not occur. Further, if the processing is performed so as to always extend in one direction of the adjacent surface, the width of the deflecting surface including the amount of extension can be managed substantially uniformly, whereby the fluctuation of the spot diameter in the main scanning direction can be suppressed.

[Description of Supporting Method of Long Cylindrical Lens] Next, the long cylindrical lens 1 according to the present invention will be described.
The supporting method 1 will be described with reference to FIG.

Since the long cylindrical lens 11 is arranged near the surface to be scanned 12, it has a long shape. Therefore, in order to prevent thermal contraction, vibration, and the like, the long cylindrical lens 11 is attached as shown in FIGS. 7A, 7B, and 7C.

That is, FIG. 11A is a side view of the long cylindrical lens 11 viewed from the incident surface side, FIG. 10B is a top view of the long cylindrical lens 11 viewed from above, and FIG. FIG. 3 is an explanatory view showing a state in which a long cylindrical lens 11 is attached from the exit surface side. Li is a light incident surface and Lo is a light exit surface.

In FIG. 11A, reference numerals 14 and 14 'denote positioning portions each serving as a lens center reference portion, each of which has a concave shape and is provided above and below the center of the long cylindrical lens 11 in the longitudinal direction (main scanning direction). Have been. In the present embodiment, the position of the long cylindrical lens 11 in the longitudinal direction is determined by fitting the positioning portion 14 and the fitting member 22 protruding from the housing 25. The fitting member 22 is provided at a position corresponding to the longitudinal center of the long cylindrical 11 in the housing 25.

The posture of the long cylindrical lens 11 in the direction of the entrance / exit surface is shown in FIGS.
6 and 17 form a pseudo three-point receiver, whereby the long cylindrical lens 11 side at the corresponding position has a predetermined flatness. The support member 16 has a linear receiving surface protruding to the height center of the long cylindrical lens 11, and the support member 17 has a linear receiving surface protruding over the height of the long cylindrical lens 11.

The vertical direction (sub-scanning direction) T of the long cylindrical lens 11 corresponds to two projections 15 provided at the longitudinal ends of the long cylindrical lens 11 shown in FIGS. Is positioned by abutting against the seat surface of the housing 25. The long cylindrical lens 11 is fixed by pressing a position facing each of the positioning portions 15, 16, and 17 with a spring member (not shown) from directions indicated by arrows 20 and 21. This embodiment has a total of four support points. Incidentally, reference numeral 19 shown in FIG. 2B denotes a chamfer for identification in the mounting direction. This is because the asymmetrical external shape prevents installation if the mounting direction is wrong.

Since the long cylindrical lens 11 is supported at both ends in the longitudinal direction, the center part is floating in the space and is easily affected by external vibration.

In the present embodiment, as a countermeasure against this, as shown in FIGS. 7A, 7B and 7C, the adhesive pedestal 26 is made independent of the fitting member 22 so as not to come into contact with the long cylindrical lens 11. And a gap between the outer frame of the long cylindrical lens 11 and the bonding pedestal 26 is about 0.4 mm or less (preferably 0.03 mm to
0.4 mm), and an adhesive 23 is applied to the position to perform slight bonding. In this way, the adhesive strength can be controlled to a level that is small enough to suppress vibration,
There is no inconsistency with the above-described positioning reference based on the fitting of the long cylindrical lens 11 based on the center and four-point support. In addition, the above-mentioned "minor" means an adhesive force controlled so as not to disturb the positioning operation. The adhesive 23 is UV cured.

Further, in the present embodiment, as shown in FIG. 9D, between the bonding pedestal 26 and the fitting member 22 (between the center reference).
Since the groove portion 27 is formed at the center, there is no need to worry that the adhesive 23 spreads between the center reference. The reason why the bonding pedestal 26 is not provided on the long cylindrical lens 11 side is to avoid complicating the outer shape of the long cylindrical lens 11 and impairing the molding stability.

As described above, in the present embodiment, the second
Long cylindrical lens 11 constituting the optical system 43 of FIG.
Positioning portions 14, 14 'are provided at the center in the longitudinal direction of
An adhesive pedestal 26 that is not in contact with the long cylindrical lens 11 is provided on the housing 25, and a gap 23 between the adhesive pedestal 26 and the long cylindrical lens 11 is filled with an adhesive 23, and the long cylindrical lens 11 is By fixing the lens to the housing 25, the influence of external vibration is prevented, and the vibration of the lens is suppressed.

Incidentally, a fitting member projecting from the long cylindrical lens may be provided, and a concave positioning portion may be provided on the bonding pedestal. Further, in an image forming apparatus using a BAE process with blank exposure, which will be described later, the effective scanning area becomes long, so that the shape of the long cylindrical lens in the main scanning direction needs to be similarly long, so that vibration is easily picked up.
From this, it can be said that the above-described method for supporting a long lens is particularly effective. In the present embodiment, the supporting method has been described by taking a long cylindrical lens as an example, but it goes without saying that other long lenses may be used.

[Description of Flange of Long Cylindrical Lens] FIGS. 8A and 8B show the shape near the longitudinal end of the long cylindrical lens and the principal ray of the light beam incident on the end. FIG. 4 is a cross-sectional view of a main part showing the relationship of FIG. FIG. 1A is a main scanning cross-sectional view, and FIG. The other end (not shown) has the same configuration.

In FIG. 10A, the long cylindrical lens 11 made of a plastic material has a lens reinforcing flange 54 at the end in the main scanning direction (integrally formed). The portion 54 protrudes from the lens surface in the optical axis direction at an inclination angle θ1. In this embodiment, the corresponding area of the lens surface through which the light beam (scanning beam) incident on the flange portion 54 is transmitted is processed into a non-mirror surface state, and in this embodiment, it is formed from a diffusion surface. This diffusion surface has a transmittance characteristic of 10% or less.

In the present embodiment, of the light beams deflected and scanned by the polygon mirror, the light beam heading toward the end of the effective scanning area (or the image forming area) passes through a position distant from the flange portion 54 and moves onto the surface to be scanned. Form an image. Further, the light beam that has been deflected and scanned is incident on a hatched portion 55 as shown in FIG. 4B, but this hatched portion 55 is a non-mirror surface region as described above and is formed by a diffusion surface. The light beam transmitted through the diffusion surface loses directivity. Therefore, even if the light beam enters the flange portion 54, the light beam is sufficiently attenuated and diffused, so that the image is not affected.

The non-specular surface area of the hatched portion 55 is not limited to the entrance surface of the lens, and may be formed on the exit surface or on both surfaces. If a non-mirror surface area is formed on both surfaces, it can function as a sufficient countermeasure against flare.

In the present embodiment, as shown in the figure, the distance d between the region of the non-specular surface portion indicated by the hatched portion 55 and the principal ray of the light beam heading toward the end of the effective scanning region (or image forming region).
Is greater than or equal to the half width of the light beam in the main scanning direction. Thus, the light beam for scanning toward the end of the effective scanning area is prevented from being applied to the non-specular area of the hatched area 55.

Further, in this embodiment, the angle θ1 formed between the flange portion 54 and the principal ray of the light beam heading toward the center of the effective scanning area is the principal ray of the light beam incident on the flange portion 54, as shown in FIG. Is set to be larger than the incident angle θ2. The angle θ1 formed between the flange portion 54 and the principal ray of the light beam heading toward the center of the effective scanning area is an angle required as a draft for forming the flange portion 54, and the angle θ1 is the optical axis of the flange portion 54. It is proportional to the length in the direction. The angle θ1 of the flange portion 54 is
If the angle is larger than the principal ray angle θ2 of the light beam incident on the light source 4, the light beam attenuated and diffused in the non-mirror surface area can escape to the outside of the effective scanning area (or image forming area). It becomes. However, flange part 5
If the angle θ1 of 4 is made unnecessarily large, the angle deviates from the original optimal value as the flange portion for reinforcing the lens, which is not necessarily preferable in terms of the lens structure.

If the non-mirror surface area of the hatched portion 55 is a surface having a diffusing action with a transmittance of 10% or less, flare light can be effectively reduced together with the diffusing property. In the present embodiment, the region of the hatched portion 55 is a diffusion surface. However, the invention is not limited to this. For example, the surface may have a light attenuation effect (for example, the non-mirror surface region is coated with black paint). Can be applied in the same manner as in the first embodiment.

[Explanation of Compact Scanning Optical Device] FIG. 9 is a sub-scan sectional view when the scanning optical device shown in FIG. 1 is compactly constructed. In the figure, the same elements as those shown in FIG. 1 are denoted by the same reference numerals.

In the same figure, the incident optical system and optical members from the polygon mirror 10 to the fθ lens system 44 are the optical box 2.
5, the first as a C-shaped mirror 52,
The optical path is routed to the lower surface of the optical box 25 by arranging the second bending mirrors 27 and 28 at right angles (C-shape). The one-dot chain line shown in FIG.
The first, second and third bending mirrors 2
7 shows a state of being bent by 7, 28, and 29. The first and second folding mirrors 27 and 28 are separately attached to the optical box 25, but one of the folding mirrors is provided with an adjusting mechanism in order to keep the right-angle error of each other within a predetermined range. And the standard of the optical box 25,
For example, the relationship with the optical box 25 is adjusted in advance so that a light beam parallel to the mounting seat surface of the polygon mirror unit is parallel and passes through a predetermined height even after passing through the C-shaped mirror 52.

The third bending mirror 29 is a mirror for bending a light beam emitted from the optical box 25 toward the photosensitive drum surface 12 side. The third folding mirror 29 is supported on the back side of the mirror 29 by three set screws, and by adjusting the three set screws, the height of the irradiation position on the photosensitive drum surface 12 (in the circumferential direction of the photosensitive drum). ), Scanning line inclination (parallelism between the photosensitive drum rotation axis and the scanning line), and overall magnification (distance from the third bending mirror to the photosensitive drum) are adjusted to predetermined performance.

The dust-proof glass 30 prevents contamination of the optical member from dust, scattered toner and the like from near the photosensitive drum surface 12. Further, the dust-proof glass 30 is detachable and can be cleaned to remove dirt. The ghost light shielding plate 41 is a member for shielding the specularly reflected light from the fθ lens system 44, and also serves as a light shielding plate and a rib for reinforcing the bottom surface of the optical box 25. The height is determined so that specularly reflected light does not escape. 32 and 33 are lids for sealing the optical box 25, respectively.

[Second Embodiment] FIG. 10A is a main scanning sectional view of a scanning optical apparatus according to a second embodiment of the present invention, and FIG.
Is a sectional view taken along the line CC 'in FIG.
It is. 1A and 1B, the same elements as those shown in FIG. 1 are denoted by the same reference numerals. 1A, the writing position detection optical system 35 for controlling the timing of the scanning start position shown in FIG. 1A is omitted.

The present embodiment is different from the first embodiment in that the incident optical system 41 is constituted by a UFS optical system and the size of the deflecting surface 10a of the polygon mirror 10 is smaller than that of the polygon mirror of the first embodiment. The difference is that the second optical system 43 is constituted by a single lens (fθ lens) 45. Other configurations and optical functions are substantially the same as those of the first embodiment, and thus, similar effects are obtained.

That is, the width of the deflecting surface 10a of the polygon mirror 10 in the main scanning direction in the present embodiment is the same as the light beam diameter of the light beam that is deflected and reflected by the polygon mirror 10 and travels toward the fθ lens 45. It is at least three times larger than the deflection surface of the polygon mirror of the optical system. Therefore, when the scanning angle is increased, the incident light beam diameter is vignetted on the deflecting surface. Therefore, for example, the scanning efficiency (duty) is about 70% at most in a device having a resolution of 600 dpi and 50 sheets. However, if the speed is further increased, the lighting time of one line itself becomes shorter, and it becomes difficult to turn off the light source. In the case of the UFS optical system, although it is not as large as that of the OFS optical system, it is essential that the light source be constantly turned on.

In FIG. 10B, the light beam emitted from the laser unit 1 passes through a position off the optical axis of the cylindrical lens 6 and is incident on the deflection surface 10a of the polygon mirror 10 in an oblique direction. In this manner, by causing the light beam to enter the deflecting surface 10a of the polygon mirror 10 in an oblique direction in the sub-scan section, the deflecting surface 10a
Even if a is perpendicular to the optical axis of the incident optical system in the main scanning section, the regular reflection light from the deflecting surface 10a does not return to the light source, so that the operation stability of the light source can be ensured. it can.

In the present embodiment, as in the first embodiment, the scanning must be performed up to the effective scanning area outside the image forming area. Therefore, as shown in FIG. The angle of incidence of the chief ray of the light beam toward the end becomes large, and the necessity for measures against flare is increasing. In the present embodiment, as in the first embodiment, the area of the lens surface (incidence surface and / or emission surface) of the lens through which the light beam entering the flange portion is transmitted is a non-mirror surface (for example, as shown by a hatched portion 55 in FIG. 8). By forming it at the (diffusion surface) portion, flare light can be suppressed regardless of the presence or absence of the flange portion.

[Image Forming Apparatus] FIG. 11 is a sectional view of a main portion in the sub-scanning direction showing an example of the configuration of an electrophotographic printer which is an image forming apparatus using the optical scanning optical apparatus of the present invention.

In the drawing, reference numeral 100 denotes the optical scanning optical device according to any one of the first and second embodiments of the present invention. 101
Denotes a photosensitive drum (photosensitive member) serving as an electrostatic latent image carrier. Above the photosensitive drum 101, a charging roller 102 for uniformly charging the surface of the photosensitive drum 101 is in contact with the surface. A light beam (light beam) 103 scanned by the optical scanning optical device 100 is applied to a charged surface on the downstream side in the rotation direction A of the photosensitive drum 101 below the contact position of the charging roller 102. It has become.

The light beam 103 is modulated on the basis of image data. By irradiating the light beam 103, an electrostatic latent image is formed on the surface of the photosensitive drum 101. The electrostatic latent image is supplied to the toner by a developing device 107 serving as a developing unit that is disposed so as to be in contact with the photosensitive drum 101 downstream of the irradiation position of the light beam 103 in the rotation direction A of the photosensitive drum 101. Developed as an image. The toner image is transferred onto a sheet 112 as a transfer material by a transfer roller 108 as a transfer unit disposed below the photosensitive drum 101 so as to face the photosensitive drum 101. The paper 112 is stored in the paper cassette 1 in front of the photosensitive drum 101 (right side in FIG. 11).
09, but can be fed manually. A paper feed roller 110 is provided at the end of the paper cassette 109.
Is provided, and the paper 11 in the paper cassette 109 is provided.
2 to the transport path.

The sheet 112 onto which the unfixed toner image has been transferred as described above is further moved to the rear of the photosensitive drum 101 (FIG. 1).
1 (left side in FIG. 1) to a fixing device as fixing means. The fixing device includes a fixing roller 113 having a fixing heater (not shown) therein, and a pressure roller 114 disposed so as to be in pressure contact with the fixing roller 113.
The unfixed toner image on the sheet 112 is fixed by heating the sheet 112 conveyed from the transfer unit while pressing the sheet 112 at the pressure contact portion between the fixing roller 113 and the pressure roller 114. Further, a paper discharge roller 116 is disposed behind the fixing roller 113, and discharges the fixed paper 112 outside the printer.

[Image Forming Apparatus Using BAE Process]
The above image forming apparatus is also suitable for use in a BAE process (background exposure type) image forming apparatus.

Here, the BAE process is called Background ar
ea exposure is an exposure process using a negative toner. The portion where the light beam is not irradiated on the surface of the photosensitive drum which is the surface to be scanned forms an image. Since the BAE process is an exposure process of an analog copying machine, it has a negative and positive relationship with an IAE (image area exposure) process which is usually applied to a scanning optical system.

Since the width of the exposure surface of the photosensitive drum in the scanning direction is wider than that of the image forming area, it is necessary to expose the area of the photosensitive drum outside the image forming area so as not to be developed. Exposure of this area is called blank exposure. In an analog machine, exposure is generally performed by an auxiliary light source. However, in a scanning optical system, a scanning width of a scanning beam is extended, and an area obtained by adding a blank exposure width to an image forming area is an optically effective scanning area. In the BAE process, the scanning width to be exposed is longer, so that the scanning efficiency is further increased, and the lens needs to be longer. Therefore, the optical system has a lens provided with a flange for reinforcement. In this apparatus, as described above, the area of the lens surface (incidence surface and / or emission surface) of the lens through which the light beam incident on the flange portion is transmitted is formed by a non-mirror surface (for example, a diffusion surface) portion, whereby the incident light beam can be reduced. It is sufficiently attenuated to effectively reduce flare light.

The use of the same BAE process for the optical scanning optical device as a digital machine as in the analog machine can replace the analog machine because consumables such as toner can use the service system and assets built by the widespread analog machine as they are. There is a merit such as smooth transition.

FIG. 12 shows a case where the present invention is applied to the BAE process.
The relationship between the effective scanning area, the image forming area, and the blank exposure area in line scanning (one line scanning width) is shown.

As shown in the figure, in the image forming apparatus using the BAE process, the effective scanning section (effective scanning area) for exposing the surface to be scanned has blank exposure areas on both sides of the image forming area, so that the scanning width becomes long. And the scanning efficiency is increased. Since the BD sensor for detecting the writing start position of the image is located upstream of the blank exposure, the time from the end of scanning to the writing start position is further shortened. For this reason, the laser needs to be constantly turned on to stabilize the light source. A light-blocking member is also required as a measure against flare. This is common to the UFS optical system and the OFS optical system, but especially when the OFS optical system and the BAE process are combined, the scanning efficiency (duty) is large, so the time of the ineffective scanning section is short, and the light source is always turned on. Required.

[0128]

According to the present invention, as described above, one or more long plastic lenses constituting the second optical system are provided with a reinforcing flange at the end in the main scanning direction, and are incident on the flange. Since the corresponding area of the entrance surface and / or the exit surface of the lens through which the transmitted light flux passes is formed on a non-mirror surface (for example, a diffusion surface), flare light can be effectively reduced,
As a result, an optical scanning optical device capable of obtaining a good image and an image forming apparatus using the same can be achieved.

The present invention is particularly effective not only in a normal UFS optical system but also in an optical scanning optical device using an OFS optical system and an image forming apparatus using a BAE process.

[Brief description of the drawings]

FIG. 1 is a sectional view of a main part according to a first embodiment of the present invention. FIG. 1 (A) is a sectional view of a main scan, FIG. 1 (B) is a sectional view of a sub-scan, and FIG.
Sectional view

FIG. 2 is an eccentric structure diagram of a long cylindrical lens.

FIG. 3 is a diagram illustrating the principle of shift adjustment of a laser unit.

FIG. 4 is an explanatory view showing a mirror adjusting mechanism.

FIG. 5 is an explanatory diagram of flare light due to the edge of a polygon mirror.

FIG. 6 is an explanatory diagram of flare light due to the edge of a polygon mirror.

FIG. 7 is an explanatory view of a supporting method of a long cylindrical lens.

FIG. 8 is an explanatory view of an end of a long cylindrical lens.

FIG. 9 is a schematic diagram of another main part of the first embodiment of the present invention.

FIG. 10 is a schematic diagram of a main part of a second embodiment of the present invention.

FIG. 11 is a sub-scan sectional view of the image forming apparatus of the present invention.

FIG. 12 is an explanatory diagram of an effective scanning area of one line of a scanning optical system in a BAE process.

DESCRIPTION OF SYMBOLS 1 ... Laser unit 2 ... Light source means (semiconductor laser) 3 ... Collimator-lens unit 4 ... Concave lens 5 ... Aperture stop 6 ... Cylindrical lens 7 ... Folding mirror 8 ... Spherical concave lens 9 ... Cylindrical lens 10 ... Deflecting means (Polygon mirror) 11 long cylindrical lens 12 scanned surface 13 light shielding member 41 incident optical system 42 first optical system 43 second optical system 44 fθ lens system 45 fθ lens 34 reflection Mirror 35 Write start position detecting optical system 36 Slit 37 Condensing lens 38 Synchronous detection element 14, 14 'Central reference 15 Reference 16 17, Reference receiving surface 18 Gate 19 Chamfer 20 Reference spring 21: Reference holding spring 22: Central reference cane member 23: UV adhesive 25: Housing 26: Adhesion stand Seat 27 ... Mirror 28 ... Mirror 29 ... Mirror 30 ... Dustproof glass 31 ... Photosensitive drum 32 ... Top cover 33 ... Bottom cover 54 ... Flange portion 55 ... Shaded portion 100 Scanning optical device 101 Photosensitive drum 102 Charging roller 103 Light beam 107 Developing device 108 Transfer Roller 109 Paper Cassette 110 Feed Roller 112 Transfer Material (Paper) 113 Fixing Roller 114 Pressure Roller 116 Discharge Roller

──────────────────────────────────────────────────続 き Continued on the front page (51) Int.Cl. ⁷ Identification symbol FI Theme coat ゛ (Reference) H04N 1/113 H04N 1/04 104A F-term (Reference) 2C362 AA42 AA45 BA85 BA90 BB33 DA28 DA29 2H045 AA01 CA03 CA63 CA88 CB63 2H087 KA19 LA22 PA03 PA17 PB03 QA03 QA06 QA18 QA21 QA25 QA32 QA41 QA46 RA08 RA12 RA13 UA01 5C051 AA02 CA07 DA01 DB02 DB22 DB24 DB30 DC04 DC05 DC07 FA01 5C072 AA03 BA15 DA02 DA04 HA13 X

Claims (22)

[Claims] 1. A light source means, a first optical system for making a light beam emitted from the light source means incident on a deflecting means, and an image of a light beam deflected and reflected by the deflecting means on an effective scanning area on a surface to be scanned. An optical scanning optical device having a second optical system, wherein the second optical system has one or more plastic lenses, and the plastic lens has a reinforcing flange at an end in the main scanning direction. An optical scanning optical device having a lens, wherein a corresponding area of an entrance surface and / or an exit surface of a lens through which a light beam incident on the flange portion passes is formed in a non-mirror surface portion. 2. The optical scanning optical device according to claim 1, wherein the non-mirror surface is a diffusion surface. 3. The optical scanning optical device according to claim 2, wherein the diffusion surface has a transmittance characteristic of 10% or less. 4. The optical scanning optical device according to claim 1, wherein the non-specular surface is a surface having an optical attenuation function. 5. An apparatus according to claim 1, wherein an interval between the non-mirror surface area and a principal ray of the light beam traveling toward an end of the effective scanning area is equal to or more than a half of a light beam width of the light beam in the main scanning direction. The optical scanning optical device according to claim 1, wherein 6. An angle formed between the flange and a principal ray of a light beam heading toward the center of the effective scanning area is larger than an incident angle of a principal ray of a light beam incident on the flange portion. The optical scanning optical device according to claim 1, wherein 7. The optical scanning optical device includes a writing position detection optical system that controls a timing of a scanning start position on the surface to be scanned by using at least a part of a light beam that scans outside an effective scanning area; 2. The optical scanning optical device according to claim 1, wherein the light source means is always turned on even when the light beam scans outside the effective scanning area. 8. An optical scanning optical system according to claim 1, wherein the light beam passing through said first optical system is obliquely incident on a deflecting surface of said deflecting means in a sub-scan section. apparatus. 9. The optical scanning optical device according to claim 1, wherein the light beam having passed through the first optical system is incident on the deflection surface from within the deflection angle of the deflection means in the main scanning section. . 10. An optical scanning optical device according to claim 1, a photosensitive member disposed on a surface to be scanned of the scanning optical device, and a light beam scanning over the photosensitive member. Developing means for developing the electrostatic latent image formed as described above as a toner image, transfer means for transferring the developed toner image to paper, and fixing means for fixing the transferred toner image to paper. An image forming apparatus comprising: 11. An image forming apparatus according to claim 10, wherein an image is formed by a BAE process. 12. A light source means, a first optical system for causing a light beam emitted from the light source means to enter a deflecting surface of the deflecting means in a state wider than a width of the deflecting surface in the main scanning direction, and the deflecting means. A second optical system that forms an image of the deflected and reflected light beam on an effective scanning area on the surface to be scanned, wherein the second optical system has one or more plastic lenses, The plastic lens has a reinforcing flange portion at an end in the main scanning direction, and a corresponding area of an entrance surface and / or an exit surface of the lens through which a light beam incident on the flange portion passes is formed in a non-mirror surface portion. Optical scanning optical device characterized by the above-mentioned. 13. The optical scanning optical device according to claim 12, wherein the non-specular surface is a diffusion surface. 14. The optical scanning optical device according to claim 13, wherein the diffusing surface has a transmittance characteristic of 10% or less. 15. The optical scanning optical device according to claim 12, wherein the non-mirror surface is a surface having an optical attenuation function. 16. The distance between the non-mirror surface area and the principal ray of the light beam heading toward the end of the effective scanning area is set to be equal to or more than half the width of the light beam in the main scanning direction. The optical scanning optical device according to claim 12, wherein 17. An angle between the flange and a principal ray of a light beam heading toward the center of the effective scanning area is greater than an incident angle of a principal ray of a light beam incident on the flange portion. The optical scanning optical device according to claim 12, wherein 18. The optical scanning optical apparatus further includes a writing position detection optical system that controls a timing of a scanning start position on the surface to be scanned by using at least a part of a light beam that scans outside an effective scanning area; 13. The light source device according to claim 12, wherein the light source is always turned on even when the light beam scans outside the effective scanning area.
An optical scanning optical device according to claim 1. 19. The optical scanning optical system according to claim 12, wherein the light beam passing through said first optical system is obliquely incident on a deflection surface of said deflection means in a sub-scan section. apparatus. 20. The optical scanning optical device according to claim 12, wherein the light beam having passed through the first optical system is incident on the deflection surface from within the deflection angle of the deflection means in the main scanning section. . 21. The optical scanning optical device according to claim 12, a photosensitive member disposed on a surface to be scanned of the scanning optical device, and a light beam scanning over the photosensitive member. Developing means for developing the electrostatic latent image formed as described above as a toner image, transfer means for transferring the developed toner image to paper, and fixing means for fixing the transferred toner image to paper. An image forming apparatus comprising: 22. The image forming apparatus according to claim 21, wherein an image is formed by a BAE process.