JP4649222B2 - Manufacturing method of imaging lens - Google Patents

Description

The present invention relates to a method for manufacturing an imaging lens having a function of suppressing the amount of light reflected from an interface on the light incident / exit surface. For example, an imaging device such as a camera or a video camera, or a liquid crystal projector or an electrophotographic device. It is suitable for projection equipment such as an optical scanning device.

  In general, an optical element that needs to suppress the amount of reflected light on the surface obtains desired reflection characteristics by laminating a single layer or a plurality of layers with an optical film having a different refractive index on its surface to a thickness of several tens to several hundreds of nm . In order to form these optical films, vacuum film formation methods such as vapor deposition and sputtering, and wet film formation methods such as dip coating and spin coating are used. Regardless of which film forming means is used, the optical element substrate must be processed and then formed into a film, which makes it difficult to manufacture and there are restrictions in reducing the cost.

  On the other hand, it is known that the amount of reflected light at the interface can be suppressed by forming a fine shape with a pitch equal to or less than the design wavelength on the surface of the optical element without using an optical film. If the fine shape can be formed on the mold using this principle, and the optical element can be manufactured together with the molding of the substrate, the manufacturing cost can be ultimately reduced.

  Conventionally, a semiconductor process is widely used as a technique for forming a fine shape called SWS (Sub Wavelength Structure), but this method has an advantage of being able to form a precisely designed SWS, but has a large area on a curved surface. However, there are many restrictions in the formation, and there is a problem that it is very difficult to manufacture inexpensively (simplely).

  On the other hand, a method of forming by using fine particles has been proposed as one of methods for easily manufacturing SWS (see, for example, Patent Documents 1 and 2).

  In Patent Document 1, when fine particles are used, it is possible to form SWS in a large area all together, but in order to form the SWS by arranging the fine particles continuously and uniformly, There is a problem that it is difficult to control the volume ratio and aspect ratio with the atmosphere, and it is difficult to obtain an ideal antireflection effect.

On the other hand, an anodic oxidation method is known as a method capable of forming SWS in a large area at low cost and controlling the aspect ratio arbitrarily. Fine pores are formed by applying a metal such as aluminum as an anode in an acidic electrolyte and oxidizing it. Utilizing this fact, a method for regularly arranging holes, a method for filling holes with different materials, and the like have been developed (see, for example, Patent Documents 3 and 4).
JP 2000-071290 A JP 2001-074919 A JP-A-2-254192 JP-A-10-121292

  When light enters the optical element, unnecessary reflected light is generated on the incident / exit surface of the optical element. A problem caused by the reflected light generated on the incident / exit surface of the optical element at this time will be described using a conventional laser beam printer (LBP) as an example. However, the problem to be solved by the present invention is a defect due to Fresnel reflection occurring at the interface where light enters and exits, and is not limited to the reflection of the solid surface.

  FIG. 8 is a sectional view (main scanning sectional view) of the main part in the main scanning direction of a conventional optical scanning device used for LBP or the like.

  In the figure, a divergent light beam emitted from a light source means 91 is made into a substantially parallel light beam or a convergent light beam by a collimator lens 92. 94 is incident. Out of the light beam incident on the cylindrical lens 94, the light beam exits as it is in the main scanning section, converges in the sub-scanning section, and converges in the vicinity of the deflecting surface 95a of the optical deflector 95 composed of a rotating polygon mirror (polygon mirror). It is formed almost as a line image.

  Then, the light beam reflected and deflected by the deflecting surface 95a of the optical deflector 95 is passed through an image forming optical means (fθ lens system) 96 having two fθ lenses 96a and 96b having fθ characteristics. By guiding the light onto the surface 97 and rotating the light deflector 95 in the direction of arrow A, the photosensitive drum surface 97 is optically scanned in the direction of arrow B (main scanning direction) to record image information. .

  In recent years, the fθ lens (optical element) constituting the imaging optical means is often formed in a free-form surface shape, and it is becoming common to produce the shape with a plastic material that is easy to manufacture.

  However, since it is difficult to apply an antireflection film to the lens surface due to technical and cost reasons, plastic lenses may omit the antireflection film, causing surface reflection on each optical surface and causing problems. was there. That is, the surface reflected light generated on the fθ lens surface from which the antireflection film is omitted may be reflected by other optical surfaces and finally reach an unintended portion of the surface to be scanned, thereby causing a ghost phenomenon.

  In particular, as shown in FIG. 8, when the optical surface (fθ lens surface) 96a1 that is relatively close to the optical deflector 95 has a concave shape and the incident light beam has an incident angle close to vertical, of the two fθ lenses, the optical surface The surface reflected light at 96a1 returns to the optical deflector 95, is reflected again by the deflecting surface (reflecting surface) 95a of the optical deflector 95, passes through the imaging optical means 96, and then an unintended portion on the photosensitive drum surface 97. In some cases, the problem of reaching ghost and becoming a ghost occurred.

An object of the present invention is to provide a method for manufacturing an imaging lens capable of obtaining uniform antireflection characteristics over the entire optical surface of an optical element having a finite curvature.

According to a first aspect of the present invention, there is provided an imaging lens manufacturing method in which a plurality of optical members having an antireflection function are formed on a refracting surface having a finite curvature, and each of the plurality of optical members has a luminous flux to be used. A method of manufacturing an imaging lens used in an optical scanning device having a convex shape smaller than a wavelength,
And the mold manufacturing process for forming the pores formed of aluminum or aluminum alloy by anodic oxidation on the surface of the mold,
Resin is injection-molded into a mold having the pores formed on the metal surface, and each of the plurality of optical members is independently formed in a normal direction of the refractive surface on the refractive surface having the finite curvature. And an element forming step to be formed .
However, when the average value of the distance between the centers of adjacent optical members is D (nm), the standard deviation is σ, and the wavelength of the luminous flux to be used is λ (nm),
D / 200 <σ <D / 10
D <λ / 2
Satisfy the condition

According to the present invention, by providing a plurality of convex optical members having an antireflection function on the surface of an optical element having a finite curvature independently in the normal direction of the surface, uniform antireflection on the entire optical surface. An imaging lens that can have properties can be achieved.

Further, according to the present invention, by mounting the imaging lens on the optical scanning device, it is possible to eliminate problems caused by the reflected light on the surface of the optical element, and it is possible to realize high brightness and energy saving by increasing the amount of transmitted light. A possible optical scanning device can be achieved.

FIGS. 1A and 1B are imaging lenses (hereinafter also referred to as “optical elements”) according to the first embodiment of the present invention . It is the schematic diagram which showed the cross section of this. FIG. 4A shows a case where the base shape of the optical surface is a convex surface, and FIG. 4B shows a case where the base shape of the optical surface is a concave surface.

  11A and 11B, reference numeral 11 denotes an optical element having a finite curvature (a finite curvature excluding infinity), and the base shape of the optical surface is formed as a convex surface or a concave surface. The optical surface of the optical element 11 in the present embodiment is composed of a refractive surface, for example.

  2A and 2B are schematic views schematically showing the arrangement of a plurality of optical pieces (optical members) in Example 1 of the present invention. FIG. 6A shows the case of the present embodiment in which a plurality of optical pieces 12 are randomly arranged on the surface of an optical element having a finite curvature, and FIG. The case where it arrange | positions in the shape of a triangular lattice on the surface of the optical element which has a finite curvature is shown.

  In this embodiment, a plurality of optical pieces are randomly arranged on the surface of an optical element having a finite curvature. That is, when a certain regularity is provided when the optical piece is arranged, there is an advantage that a sharp antireflection characteristic with respect to the wavelength is obtained, but there is a possibility that the optical characteristic has an angle dependency. For example, when regularly arranged in a triangular lattice shape as shown in FIG. 2B, the interval between the optical pieces is the shortest along the array and the longest in the direction of 30 degrees. The antireflection characteristic shifts depending on the incident direction.

Therefore, in the present embodiment, among the plurality of optical pieces 12, when the average value of the center distance between adjacent optical pieces 12 is D and the standard deviation is σ,
D / 200 <σ <D / 10 (1)
Is set to satisfy the following conditions. That is, when the standard deviation σ of the distance between the centers of the optical pieces is 0.5% or more of the average value D, an antireflection characteristic independent of the incident direction of light is obtained, and the standard deviation σ of the distance between the centers of the optical pieces is obtained. Is 10% or less of the average value D, it is possible to ensure antireflection characteristics for a short wavelength region. At this time, the plurality of optical pieces 12 mainly include independent optical pieces, but may include bonded optical pieces.

The average value D and the standard deviation σ of the distance between the centers of the adjacent optical pieces refer to the average value and the standard deviation of the distances between the centers when approximately arranged in a triangular lattice shape. That is, the center-to-center distance d _i of the optical piece i the average of the center-to-center distance for the nearest six optical pieces, calculates the distance between the centers to the optical piece of the measurement area, it based on equation (2 ) And the average deviation D and standard deviation σ are obtained as expressed by equation (3).

  FIG. 3A is a schematic diagram schematically showing a cross section of a plurality of optical pieces according to the first embodiment of the present invention.

  Reference numeral 12 denotes a fine optical piece (convex shape portion), which has a reflection preventing function and is provided in a random manner on the surface (base shape is concave or convex) of the optical element 11 having a finite curvature. The plurality of optical pieces 12 each have substantially the same convex shape, and the thickness thereof is substantially uniform as the distance from the surface of the optical element 11 increases, and is formed independently in the normal direction of the surface.

  Here, the antireflection function is a function of reducing the reflectance of the surface on which the optical piece is arranged compared to the reflectance of the mirror surface, preferably less than 1/2, more preferably less than 1/4. Call it. Further, the convex shape refers to a shape in which a part projects, and includes, for example, a cylindrical shape, a polygonal column shape, and the like.

The plurality of optical pieces 12 include independent optical pieces, but may include joined optical pieces. The plurality of optical pieces 12 are formed by molding on the surface of an optical element having a finite curvature.

In this embodiment, as described above, the plurality of optical pieces 12 having substantially the same convex shape are formed on the surface of the optical element having a finite curvature independently in the normal direction of the surface, thereby the optical surface. Uniform anti-reflective properties are expressed on the entire surface.

In order to express an excellent antireflection function in this embodiment, when the wavelength of the light beam used is λ,
D <λ / 2 (4)
Is set to satisfy the following conditions. That is, it is particularly desirable that the interval between the adjacent optical pieces is ½ or less of the wavelength λ used, which is said not to generate 0th-order diffracted light.

  Conditional expression (4) defines the upper limit of the average value D of the distance between the centers of the adjacent optical pieces 12. If the upper limit of conditional expression (4) is exceeded, the optical surface is uniformly excellent in antireflection characteristics. It is not good because it becomes difficult to express. Moreover, there is no functional restriction on the lower limit, and the lower limit may be small as long as the volume ratio between the optical piece and the atmosphere described later is appropriate.

  The wavelength used here refers to the wavelength of light transmitted through the optical element or reflected by the optical element, and refers to a wavelength intended to suppress the amount of reflected light. For example, when it is desired to transmit visible light through an optical element and suppress the amount of reflected light with a wavelength of 600 nm or less, it is desirable that the wavelength used is 600 nm and the interval between adjacent optical pieces is 300 nm or less. Alternatively, in the laser beam printer exemplified in the above-described problem, 780 nm laser light is used, and the interval between adjacent optical pieces is preferably 390 nm or less.

    In this embodiment, as described above, a plurality of optical pieces 12 having substantially the same convex shape are formed on the surface of an optical element having a finite curvature independently in the normal direction of the surface, and adjacent optical pieces. Are set so that the average value D and the standard deviation σ of the center distances satisfy the above conditional expressions (1) and (4). As a result, a uniform antireflection characteristic is exhibited over the entire optical surface regardless of the incident direction of light.

  In general, when two substances having different refractive indexes at a pitch shorter than the wavelength are mixed, the refractive index (hereinafter referred to as equivalent refractive index) n12 of the mixed area is the refractive index (n1, n2) of the two substances. By each volume (ff1, ff2) occupying per unit volume, it can be expressed approximately by equation (5).

n12 = ff1 × n1 + ff2 × n2 (5)
At this time, when there are only two substances in the mixed area ff1 + ff2 = 1 (6)
In the case where light is incident vertically from the substance 1 to the substance 2 or from the substance 2 to the substance 1, the equivalent refractive index n12 of the mixed region is

When it is, the antireflection effect becomes the highest.

  For example, when the optical piece is in contact with the atmosphere, assuming that the refractive index of the substance constituting the optical piece is n, the ratio ff and the equivalent refractive index n12 occupying the unit volume of the projection having the highest antireflection effect are given by the following formula (8 ) And formula (9).

n12 = ff × (n−1) +1 (9)
If the optical surface on which the optical piece is formed is the outermost surface in contact with the atmosphere, and the refractive index n of the material constituting the optical piece is 1.56, in order to obtain the maximum antireflection effect for normal incidence, From the formula (8), the volume ratio occupied by the optical piece is particularly preferably about 44%. The optimum value of the volume ratio is set as appropriate not only by the refractive index of the material constituting the optical piece, but also by the incident angle and polarization of light, but empirically, the optical piece is constituted by a volume ratio of 38 to 65%. Is particularly preferable in order to obtain desired antireflection characteristics.

By thus in this embodiment, in which a plurality of optical pieces of convex shape having a reflection preventing function on a surface of an optical element having a finite curvature as described above, i.e., a wavelength equal to or less than the pitch of the light beam to be used By providing a fine-shaped optical piece , a uniform antireflection characteristic is exhibited over the entire optical surface.

  FIGS. 3B to 3E are schematic views schematically showing cross sections of a plurality of optical pieces related to Example 2 of the present invention.

  In this embodiment, the difference from the first embodiment is that the optical piece is formed in a shape that becomes narrower in the radial direction as it moves away from the surface of the optical element having a finite curvature. Other configurations and optical actions are substantially the same as those in the first embodiment, and the same effects are obtained.

  That is, FIG. 4B shows a state where the radial thickness of the optical piece is narrowed toward the tip, and FIG. 4C is a diagram where the radial thickness of the optical piece is directed toward the tip. FIG. 4D shows a state in which the thickness of the optical piece in the radial direction is tapered toward the tip, and FIG. Shows a state in which the thickness of the optical piece in the radial direction narrows in a multi-step shape toward the tip.

  The plurality of optical pieces 12 in the present embodiment are randomly arranged on the surface of the optical element having a finite curvature (the base shape is concave or convex) as in the first embodiment. It is formed independently in the line direction. Similarly to the first embodiment, the average value D and the standard deviation σ of the center distance between adjacent optical pieces 12 are set so as to satisfy the conditional expressions (1) and (4).

In this embodiment, as described above, the optical piece 12 is formed so as to become narrower in the radial direction (toward the tip) as it moves away from the surface of the optical element, and an excellent reflection is achieved by changing the equivalent refractive index n12 toward the tip. Preventive properties are obtained.
Refractive index change at the boundary surface in the height direction of the optical piece because the optical piece has the same thickness in the height direction or a structure in which the radial direction becomes thicker toward the tip, and becomes narrower toward the tip. And an excellent antireflection effect can be obtained.

  Further, in this embodiment, as shown in FIG. 3C, the dimension in the radial direction of the optical piece 12 is formed in a shape that becomes thinner stepwise as the distance from the surface of the optical element increases. That is, an excellent antireflection characteristic can be obtained by changing the equivalent refractive index from the substance 1 to the substance 2 for each step. In addition, it is preferable that the means for forming a fine shape whose radial direction becomes narrower toward the tip can be formed relatively easily by thinning in a step shape.

  Further, in this embodiment, as shown in FIG. 3D, the radial dimension of the optical piece 12 is formed so as to become tapered as the distance from the surface of the optical element increases. That is, a particularly excellent antireflection characteristic can be obtained by changing the equivalent refractive index from the substance 1 to the substance 2 in a stepless manner.

  Further, in this embodiment, as shown in FIG. 3E, the radial dimension of the optical piece 12 is formed in a shape that becomes thinner in a multi-step shape as the distance from the surface of the optical element increases. That is, an excellent antireflective characteristic can be obtained by changing the equivalent refractive index from the substance 1 to the substance 2 at every multi-step.

In this embodiment, the antireflection function of the plurality of optical pieces in FIGS. 3B, 3C, 3D, and 3E is compared to FIG.
(a) Incidence angle characteristics are improved,
(b) The wavelength range of the antireflection characteristic is widened.
It has the feature.

  Next, the manufacturing method of the optical element of this invention is demonstrated.

  In addition, the manufacturing method of this invention is not limited to the manufacturing method shown below. Although the present invention is intended to prevent reflection of a 780 nm P-polarized laser, the anti-reflection characteristics of the optical element obtained by the present invention are not limited to single-wavelength lasers, but are visible light, ultraviolet light, and infrared light. It can also be applied to.

  In the present invention, an optical piece is formed by transferring the pores using the mold, and a mold manufacturing process for forming pores formed when anodizing aluminum or aluminum alloy on the mold surface. An optical element is manufactured using an element molding process.

  Here, anodic oxidation is performed by immersing aluminum or an aluminum alloy as a positive electrode in an electrolyte solution composed of sulfuric acid, oxalic acid, and phosphoric acid, and connecting a DC power source to the negative electrode that has been similarly immersed to energize. This is a technique in which aluminum or an aluminum alloy is oxidized to form submicron-order pores in a direction perpendicular to the surface.

  It is known that the pitch and the pore diameter of the pores can be controlled by appropriately selecting conditions. By appropriately selecting the conditions of the anodic oxidation method, SWS can be formed in a short time and at low cost by forming desired pores all over the mold surface.

Molding is performed as a means for transferring the pores formed in the mold. More specifically, any molding means such as injection, replica, press, and casting may be used, but injection and press molding that can efficiently transfer and form SWS together with the substrate are particularly desirable. Also, when releasing from the mold, the direction of the optical piece and the release direction are not necessarily parallel, but before the optical piece can be deformed to some extent, for example, before the material constituting the optical piece is completely solidified. It can be easily released by molding.
[Production Method 1]
The optical element manufacturing method 1 will be described.

First, a mold having a free curved surface for forming an fθ lens (optical element) is prepared as an imaging lens, and a primer layer and an aluminum layer are uniformly formed on the free curved surface in this order by sputtering, and the free curved surface covered with aluminum. Got. Then, a positive electrode was attached to a part of the surface excluding the free curved surface, and the entire mold was covered with a masking tape so that only the free curved surface was exposed.

  Next, it was immersed with a negative electrode in a 5 wt% phosphoric acid aqueous solution adjusted to 10 ° C. Thereafter, 120 V was applied and energized by a direct current power source, and energization was performed until the energization flow rate was sufficiently weak, thereby obtaining a mold having a random arrangement and pores perpendicular to the surface. Further, it was immersed in a 5% by weight phosphoric acid aqueous solution at room temperature, and the hole diameter was expanded while gradually etching to obtain a mold for an fθ lens having a desired hole shape.

  The fθ lens mold thus obtained is observed with a scanning electron microscope, the center position of the pores is obtained by image processing, and the average value D of the center-to-center distances with the six nearest pores is obtained. As a result, the average value D of the distance between the centers of adjacent pores was about 300 nm, and the standard deviation σ was about 10 nm.

The mold manufactured by the above procedure is placed on the entrance surface side and the exit surface side of an injection molding machine (Sumitomo Heavy Industries, Ltd .: SS180), and a cycloolefin polymer (Nippon Zeon Corporation) is injection molded to produce an fθ lens. Got. At this time, the molten resin temperature was 270 ° C., and the holding pressure at the time of resin injection was 700 kg / cm ² .

  When the fθ lens thus obtained was observed with a scanning electron microscope, as shown in FIG. 4, columnar optical pieces randomly arranged over the entire curved surface were observed, and each columnar optical piece was a surface method. It was confirmed that he was standing in the direction of the line.

  Further, the center position of the optical piece is obtained by image processing from an electronic image obtained by looking down the optical piece vertically, and the average of the distances D between the centers of the six most recent columnar optical pieces is obtained. The average value D of the distance between the centers of the pieces is about 300 nm, the standard deviation σ is about 10 nm (these satisfy the conditional expressions (1) and (4)), and the mold pores are transferred. It was confirmed that

Further, when the height of the columnar optical piece was measured with an atomic force microscope, it had the cross section of FIG. 3B, the thickness of the optical piece was almost uniform toward the tip, and the average height was about 160 nm. The volume ratio of the optical piece was approximately 56%. Therefore, the reflectance at the time of vertical incidence of P-polarized light with a wavelength of 780 nm was measured using a spectrophotometer and found to be 1.6%.
[Comparative Example 1]
Next, Comparative Example 1 for manufacturing methods 1 and 2 will be described.

  A mold having a free curved surface for forming an fθ lens (optical element) was prepared, and injection molding was performed in the same manner as in Production Methods 1 and 2, and an fθ lens having a free curved mirror surface was obtained.

When the optical element thus obtained was observed with a scanning electron microscope, only a smooth surface was observed, and the reflectance at the time of vertical incidence of P-polarized light with a wavelength of 780 nm was measured with a spectrophotometer. %Met.
[Production Method 2]
Next, the optical element manufacturing method 2 will be described.

  First, a mold having a free curved surface for forming an fθ lens (optical element) was prepared, and a primer layer and an aluminum layer were uniformly formed on the free curved surface in this order by sputtering to obtain a free curved surface covered with aluminum. Then, a positive electrode was attached to a part of the surface excluding the free curved surface, the entire mold was covered with a masking tape so that only the free curved surface was exposed, and the portions other than the free curved surface were insulated and waterproofed by covering.

  Then, half of the aluminum film thickness is anodized and then melted to widen the pore diameter, and then anodized again and the remaining aluminum film is anodized to make the pore diameter narrower in a step shape. Formed.

  First, it was immersed together with a negative electrode in a 5 wt% phosphoric acid aqueous solution whose temperature was adjusted to 10 ° C. as anodization, and a DC constant voltage of 120 V was applied for a certain period of time to form pores to about half of the aluminum film thickness. Next, the pore diameter was widened by immersing in a 5 wt% phosphoric acid aqueous solution at room temperature for 1 hour and etching. When immersed in a 5% by weight phosphoric acid aqueous solution adjusted to 10 ° C. with a negative electrode, a DC constant voltage of 120 V was applied, and the energization current was sufficiently weakened. A mold surface for an fθ lens was obtained that had a hole diameter that was vertical and had two steps in the depth direction.

The mold manufactured by the above procedure is placed on the entrance surface side and the exit surface side of an injection molding machine (Sumitomo Heavy Industries, Ltd .: SS180), and a cycloolefin polymer (Nippon Zeon Corporation) is injection molded to produce an fθ lens. Got. At this time, the molten resin temperature was 270 ° C., and the holding pressure at the time of resin injection was 700 kg / cm ² .

  When the fθ lens thus obtained was observed with a scanning electron microscope, an optical piece having a thickness reduced in two stages as shown in FIG. Observed, it was confirmed that each optical piece stood toward the normal direction of the surface. In addition, the center position of the optical piece was obtained by image processing from an electronic image obtained by looking down the optical piece vertically, and the average of the distances between the centers of the six most recent optical pieces was obtained. The average distance D was about 300 nm, and the standard deviation σ was about 12 nm (this satisfies the conditional expressions (1) and (4)).

Furthermore, when the height of the columnar optical piece was measured with an atomic force microscope, the average height was about 170 nm. Therefore, when the reflectance at the time of perpendicular incidence of P-polarized light was measured using a spectrophotometer, it was 1.5%.
[Production Method 3]
Next, the optical element manufacturing method 3 will be described.

  First, a mold having a free curved surface for forming an fθ lens (optical element) was prepared, and a primer layer and an aluminum layer were uniformly formed on the free curved surface in this order by sputtering to obtain a free curved surface covered with aluminum. Then, a positive electrode was attached to a part of the surface excluding the free curved surface, the entire mold was covered with a masking tape so that only the free curved surface was exposed, and the portions other than the free curved surface were insulated and waterproofed by covering.

Thereafter, anodization and etching were alternately repeated to form pores having a substantially tapered pore diameter on the mold surface.
First, it is immersed with a negative electrode in a 5% by weight phosphoric acid aqueous solution adjusted to 10 ° C. as anodization, and a constant DC voltage of 120 V is applied for a certain period of time to form pores of about one-tenth of the aluminum film thickness. It was. Next, as an etching, the pore diameter was widened by immersing in a 5% by weight phosphoric acid aqueous solution at room temperature for 10 minutes to dissolve. The above anodic oxidation and etching steps were repeated a total of 10 times to obtain a mold surface for an fθ lens having a random arrangement and a tapered shape with a substantially tapered diameter in the depth direction.

The mold manufactured by the above procedure is placed on the entrance surface side and the exit surface side of an injection molding machine (Sumitomo Heavy Industries, Ltd .: SS180), and a cycloolefin polymer (Nippon Zeon Corporation) is injection molded to produce an fθ lens. Got. At this time, the molten resin temperature was 270 ° C., and the holding pressure at the time of resin injection was 700 kg / cm ² .

  The fθ lens thus obtained was observed with a scanning electron microscope. As a result, an optical piece having a tapered thickness was obtained as shown in FIG. 3D, which was randomly arranged over the entire curved surface. Observed, it was confirmed that each optical piece stood toward the normal direction of the surface. In addition, the center position of the optical piece was obtained by image processing from an electronic image obtained by looking down the optical piece vertically, and the average of the distances between the centers of the six most recent optical pieces was obtained. The average distance D was about 300 nm, and the standard deviation σ was about 8 nm (this satisfies the conditional expressions (1) and (4)).

Furthermore, when the height of the columnar optical piece was measured with an atomic force microscope, the average height was about 180 nm. Therefore, when the reflectance at the time of perpendicular incidence of P-polarized light was measured using a spectrophotometer, it was 1.5%.
[Optical equipment]
The optical element of the present invention can be applied to imaging devices such as cameras and video cameras, or projection devices such as liquid crystal projectors and displays, and optical scanning devices for electrophotographic devices. For example, in an optical scanning device of an electrophotographic apparatus, if an fθ lens in which a plurality of optical pieces are formed on both the entrance surface and the entrance / exit surface of an fθ lens that constitutes a conjugating optical means, good reflection characteristics can be obtained.
[Optical scanning device]
FIG. 5 is a schematic view of a main part when an fθ lens including an optical element manufactured by any one of the manufacturing methods 1 to 4 is applied to an imaging optical means of an optical scanning device such as an electrophotographic apparatus.

  In the figure, reference numeral 1 denotes light source means (semiconductor laser), which is composed of, for example, a single beam laser or a multi-beam laser. Reference numeral 2 denotes a collimator lens, which converts a light beam emitted from the light source means 1 into a substantially parallel light beam. Reference numeral 3 denotes an aperture stop which shapes the beam shape by limiting the passing light flux. A cylindrical lens 4 has a predetermined power only in the sub-scanning direction, and the light beam that has passed through the aperture stop 3 is substantially applied to a deflection surface (reflection surface) 5a of an optical deflector 5 to be described later in the sub-scan section. It is formed as a line image.

  An optical deflector 5 as a deflecting means is composed of, for example, a four-sided polygon mirror (rotating polygon mirror), and is rotated at a constant speed in the direction of arrow A in the figure by a driving means (not shown) such as a motor. ing.

  Reference numeral 6 denotes an fθ lens system as an imaging optical means having a condensing function and an fθ characteristic, and the first and second fθ lenses 6a manufactured by any one of the manufacturing methods 1 to 4 described above. 6b, and a plurality of optical pieces (convex-shaped portions) 12 are formed on the incident surfaces and exit surfaces 6a1, 6a2, 6b1, 6b2 of the first and second fθ lenses 6a, 6b. A light beam based on the image information reflected and deflected by the deflector 5 is imaged on the photosensitive drum surface 7 as the scanned surface, and the deflection surface 5a of the optical deflector 5 and the photosensitive drum surface 7 are within the sub-scanning section. By having a conjugate relationship between them, a tilt correction function is provided.

  Reference numeral 7 denotes a photosensitive drum surface as a surface to be scanned.

  In this embodiment, the light beam emitted from the semiconductor laser 1 is converted into a substantially parallel light beam by the collimator lens 2, the light beam (light quantity) is limited by the aperture stop 3, and is incident on the cylindrical lens 4. Of the substantially parallel light beam incident on the cylindrical lens 4, the light beam is emitted as it is in the main scanning section. In the sub-scan section, the light beam converges and forms a substantially linear image (a linear image long in the main scanning direction) on the deflecting surface 5a of the optical deflector 5. The light beam reflected and deflected by the deflecting surface 5a of the optical deflector 5 is imaged in a spot shape on the photosensitive drum surface 7 via the first and second fθ lenses 6a and 6b. By rotating in the A direction, the photosensitive drum surface 7 is optically scanned in the arrow B direction (main scanning direction) at a constant speed. As a result, an image is recorded on the photosensitive drum surface 7 as a recording medium.

  With the above configuration, high luminance and energy saving can be realized by suppressing the amount of reflected light on the incident surface of the fθ lens (optical element) to prevent problems such as ghosts or increasing the amount of transmitted light on the exit surface. Furthermore, the above configuration makes it possible to use an inexpensive fθ lens having an antireflection function, and in particular, in an optical apparatus equipped with a plurality of the same elements, the cost can be reduced according to the number.

  In the above optical scanning device, the plurality of optical pieces 12 are formed on the entrance surfaces and exit surfaces 6a1, 6a2, 6b1, 6b2 of the first and second fθ lenses 6a, 6b. One fθ lens may be used, and it is not limited to both the entrance surface and the exit surface, and may be one surface.

[Image forming apparatus]
FIG. 6 is a cross-sectional view of a main part in the sub-scanning direction showing an embodiment of the image forming apparatus of the present invention using the optical scanning device having the configuration shown in FIG. In the figure, reference numeral 104 denotes an image forming apparatus. Code data Dc is input to the image forming apparatus 104 from an external device 117 such as a personal computer. The code data Dc is converted into image data (dot data) Di by a printer controller 111 in the apparatus. The image data Di is input to the optical scanning device 100 having the configuration shown in FIG. The light scanning device 100 emits a light beam 103 modulated in accordance with the image data Di, and the light beam 103 scans the photosensitive surface of the photosensitive drum 101 in the main scanning direction.

  The photosensitive drum 101 serving as an electrostatic latent image carrier (photoconductor) is rotated clockwise by a motor 115. With this rotation, the photosensitive surface of the photosensitive drum 101 moves in the sub-scanning direction perpendicular to the main scanning direction with respect to the light beam 103. Above the photosensitive drum 101, a charging roller 102 for uniformly charging the surface of the photosensitive drum 101 is provided so as to contact the surface. The surface of the photosensitive drum 101 charged by the charging roller 102 is irradiated with a light beam 103 scanned by the optical scanning device 100.

  As described above, the light beam 103 is modulated based on the image data Di, and 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 developed as a toner image by a developing unit 107 disposed so as to contact the photosensitive drum 101 further downstream in the rotation direction of the photosensitive drum 101 than the irradiation position of the light beam 103.

  The toner image developed by the developing unit 107 is transferred onto a sheet 112 as a transfer material by a transfer roller 108 disposed below the photosensitive drum 101 so as to face the photosensitive drum 101. The paper 112 is stored in the paper cassette 109 in front of the photosensitive drum 101 (on the right side in FIG. 6), but can be fed manually. A paper feed roller 110 is provided at the end of the paper cassette 109, and feeds the paper 112 in the paper cassette 109 into the transport path.

  As described above, the sheet 112 on which the unfixed toner image has been transferred is further conveyed to a fixing device behind the photosensitive drum 101 (left side in FIG. 6). 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, and the sheet conveyed from the transfer unit. The unfixed toner image on the paper 112 is fixed by heating 112 while applying pressure 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 the fixed paper 112 is discharged out of the image forming apparatus.

  Although not shown in FIG. 6, the print controller 111 controls not only the data conversion described above, but also controls each part in the image forming apparatus including the motor 115, a polygon motor in the optical scanning apparatus described later, and the like. I do.

  When this image forming apparatus was used to repeatedly output a pattern image and a photographic image, no ghost phenomenon occurred and there was no problem in durability.

[Color image forming apparatus]
FIG. 7 is a schematic view of a main part of a color image forming apparatus according to an embodiment of the present invention using a plurality of optical scanning devices having the configuration shown in FIG. This embodiment is a tandem type color image forming apparatus in which four optical scanning devices are arranged side by side and image information is recorded on a photosensitive drum surface as an image carrier in parallel. In FIG. 7, 60 is a color image forming apparatus, 61, 62, 63, and 64 are optical scanning devices each having the structure shown in FIG. 5, 21, 22, 23, and 24 are photosensitive drums as image carriers, respectively. , 32, 33 and 34 are developing units, and 51 is a conveyor belt.

  In FIG. 7, the color image forming apparatus 60 receives R (red), G (green), and B (blue) color signals from an external device 52 such as a personal computer. These color signals are converted into C (cyan), M (magenta), Y (yellow), and B (black) image data (dot data) by a printer controller 53 in the apparatus. These image data are input to the optical scanning devices 61, 62, 63 and 64, respectively. From these optical scanning devices, light beams 41, 42, 43, and 44 modulated according to each image data are emitted, and the photosensitive surfaces of the photosensitive drums 21, 22, 23, and 24 are caused by these light beams. Scanned in the main scanning direction.

  The color image forming apparatus according to the present embodiment has four optical scanning devices (61, 62, 63, 64) arranged in each color of C (cyan), M (magenta), Y (yellow), and B (black). Correspondingly, image signals (image information) are recorded on the photosensitive drums 21, 22, 23, and 24 in parallel, and a color image is printed at high speed.

  As described above, the color image forming apparatus in this embodiment uses the light beams based on the respective image data by the four optical scanning devices 61, 62, 63, and 64, and the corresponding photosensitive drums 21 and 22 respectively corresponding to the latent images of the respective colors. , 23, 24 on the surface. Thereafter, a single full color image is formed by multiple transfer onto a recording material.

  As the external device 52, for example, a color image reading device including a CCD sensor may be used. In this case, the color image reading apparatus and the color image forming apparatus 60 constitute a color digital copying machine.

The figure which represented typically the cross section of the optical element of Example 1 of this invention The figure which represented typically the arrangement | sequence of the optical piece which concerns on Example 1 of this invention. The figure which represented typically the cross section of the optical piece which concerns on Example 2 of this invention. The figure which observed the ftheta lens with the scanning electron microscope Sectional drawing of the principal part of the optical scanning device carrying the optical element of this invention Cross-sectional view of essential parts of the image forming apparatus of the present invention Sectional drawing of the principal part of the color image forming apparatus of this invention Sectional view of the main part of a conventional optical scanning device

Explanation of symbols

1 Light source means (semiconductor laser)
DESCRIPTION OF SYMBOLS 2 Collimator lens 3 Aperture stop 4 Cylindrical lens 5 Optical deflector 5a Deflection surface 6 Imaging optical means 6a, 6b f (theta) lens 6a1, 6b1 Incident surface 6a2, 6b2 Output surface 7 Scanned surface 11 Optical element 12 Optical piece 100 Optical scanning device DESCRIPTION OF SYMBOLS 101 Photosensitive drum 102 Charging roller 103 Light beam 104 Image forming apparatus 107 Developing apparatus 108 Transfer roller 109 Paper cassette 110 Paper feed roller 111 Printer controller 112 Transfer material (paper)
DESCRIPTION OF SYMBOLS 113 Fixing roller 114 Pressure roller 115 Motor 116 Paper discharge roller 117 External apparatus 61, 62, 63, 64 Optical scanning device 21, 22, 23, 24 Image carrier (photosensitive drum)
31, 32, 33, 34 Developer 41, 42, 43, 44 Light beam 51 Paper transport path 52 External device 53 Printer controller 60 Color image forming apparatus

Claims (1)

A plurality of optical members having an antireflection function are formed on a refracting surface having a finite curvature, and each of the plurality of optical members is used in an optical scanning device having a convex shape smaller than the wavelength of a light beam to be used. An image lens manufacturing method comprising:
And the mold manufacturing process for forming the pores formed of aluminum or aluminum alloy by anodic oxidation on the surface of the mold,
Resin is injection-molded into a mold having the pores formed on the metal surface, and each of the plurality of optical members is independently formed in a normal direction of the refractive surface on the refractive surface having the finite curvature. And an element forming step for forming an imaging lens .
However, when the average value of the distance between the centers of adjacent optical members is D (nm), the standard deviation is σ, and the wavelength of the luminous flux to be used is λ (nm),
D / 200 <σ <D / 10
D <λ / 2
Satisfy the condition