WO2004113971A1 - 光学素子 - Google Patents
光学素子 Download PDFInfo
- Publication number
- WO2004113971A1 WO2004113971A1 PCT/JP2004/008822 JP2004008822W WO2004113971A1 WO 2004113971 A1 WO2004113971 A1 WO 2004113971A1 JP 2004008822 W JP2004008822 W JP 2004008822W WO 2004113971 A1 WO2004113971 A1 WO 2004113971A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- resin layer
- resin
- optical element
- refractive index
- environmental resistance
- Prior art date
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/18—Diffraction gratings
- G02B5/1814—Diffraction gratings structurally combined with one or more further optical elements, e.g. lenses, mirrors, prisms or other diffraction gratings
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B29—WORKING OF PLASTICS; WORKING OF SUBSTANCES IN A PLASTIC STATE IN GENERAL
- B29D—PRODUCING PARTICULAR ARTICLES FROM PLASTICS OR FROM SUBSTANCES IN A PLASTIC STATE
- B29D11/00—Producing optical elements, e.g. lenses or prisms
- B29D11/0073—Optical laminates
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/0018—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 with means for preventing ghost images
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B3/00—Simple or compound lenses
- G02B3/02—Simple or compound lenses with non-spherical faces
- G02B3/08—Simple or compound lenses with non-spherical faces with discontinuous faces, e.g. Fresnel lens
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10T—TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
- Y10T428/00—Stock material or miscellaneous articles
- Y10T428/24—Structurally defined web or sheet [e.g., overall dimension, etc.]
- Y10T428/24479—Structurally defined web or sheet [e.g., overall dimension, etc.] including variation in thickness
- Y10T428/24612—Composite web or sheet
Definitions
- the present invention relates to an optical element such as a diffractive lens having predetermined optical characteristics by laminating two or more layers of resin on a base material.
- a resin layer having a different refractive index from that of the base material is formed on the surface of a base material such as glass, and the interface between the base material and the resin layer is formed into a special shape, so that optical elements such as a diffraction lens as a whole are formed.
- An optical element having such characteristics is known. However, in such an optical element, there is a problem in that the processing of the surface of the base material such as glass has to be performed, and the processing is troublesome.
- a first resin layer having a predetermined surface shape pattern is formed on the surface of a base material such as glass, and the first resin layer is formed thereon.
- Fig. 6 shows an example.
- FIG. 6 is a cross-sectional view of the force S, which is omitted because hatching is difficult to understand.
- a first resin layer 12 is formed on a transparent substrate 11 such as glass as a base material via a silane coupling treatment layer. Then, a pattern is formed on the surface of the resin layer 12 so as to give optical characteristics such as a diffraction lens.
- a silane coupling treatment layer On top of the resin layer 12 is further formed a silane coupling treatment layer, on which a second resin layer 12 having a different refractive index from that of the first resin layer 12 is formed.
- the resin layer 13 of the layer is formed.
- the difference in the refractive index between the first resin layer 12 and the second resin layer 13 and the shape of the pattern formed between the two layers have predetermined optical characteristics.
- the formation of the silane coupling layer is not always an essential condition.
- FIG. 6 shows a transparent substrate 11 as a base material and two resin layers 12 and 13. If necessary, the refractive index between the layers may be formed on the resin layer 13. It is also possible to provide one or more resin layers different from each other.
- An example of such an optical element is described in, for example, Japanese Patent Application Laid-Open No. Hei 9-127732.
- the optical element is designed based on the same idea as that in which a single resin layer is formed on the base material.
- Glass which is a commonly used base material, has a higher refractive index than resin, so if designed with the same concept, the two-layer resin with the higher refractive index is closer to the base material. It was designed to expose the smaller refractive index to the outside air, and was not designed in consideration of environmental resistance. As a result, the resin layer formed on the uppermost layer (surface opposite to the base material) and exposed to the outside air may be damaged, or the adhesion of the antireflection film may be poor.
- a step called “draft” may be formed on the step structure portion of the diffractive optical surface in order to improve the releasability between the mold and the molded resin. Even in such a case, the above-described invention has a problem that flare is generated at a draft portion. Disclosure of the invention
- the present invention has been made in view of such circumstances, and an object of the present invention is to provide an optical element formed by laminating a plurality of resin layers on a base material and having good environmental resistance. This is the first purpose. Also, when the draft is provided, A second object is to provide a diffractive optical element that is less likely to generate flare on a folding optical surface.
- a first resin layer is formed on a base material, and a second resin layer having a different refractive index from the first resin layer is formed thereon. And, if necessary, a resin layer having a different refractive index from that of the resin layer formed thereunder is sequentially formed thereon, and a predetermined shape is provided at an interface between the resin layers, thereby providing a desired shape.
- Resin is easier to process than glass and other base materials. For example, when two resin layers are superimposed and given the desired characteristics depending on the shape of the interface, one of the upper layers (the opposite side to the base material) However, it is easy to have the same characteristics by reversing the shape of the interface.
- the present invention makes use of this fact, and the resin constituting the resin layer formed on the uppermost surface (the side opposite to the base material) is the most excellent in environmental resistance among the resins forming the resin layer. To make sure that By doing so, the surface of the resin layer that comes into direct contact with the outside air becomes the surface of the resin having the highest environmental resistance, and thus the optical element can have excellent environmental resistance.
- a second invention for achieving the first object is the first invention, wherein the environmental resistance is a hardness of a resin. Hardness (especially pencil hardness) is used as an index of environmental resistance, and by using a resin having high hardness as the resin constituting the resin layer formed on the uppermost surface, the surface of the resin is damaged. A difficult optical element can be obtained.
- a third invention for achieving the first object is the first invention, wherein the environmental resistance is a dimensional change rate due to water absorption. Things.
- a dimensional change rate due to water absorption is used, and a resin having a small change rate is used as a resin constituting the resin layer formed on the uppermost surface, thereby providing an optical element having good moisture resistance. be able to.
- a fourth invention for achieving the first object is the first invention, wherein the environmental resistance is a gel fraction.
- a gel fraction weight ratio before and after immersion in methyl ethyl ketone at 70 ° C for 6 hours
- a resin having a large gel fraction is formed on the uppermost surface.
- the resin constituting the resin layer it is possible to obtain an optical element that is hardly scratched on its surface and has good moisture resistance.
- a fifth invention for achieving the first object is the first invention, wherein the environmental resistance is a glass transition point.
- a glass transition point as an index of environmental resistance and using a resin having a high glass transition point as the resin constituting the resin layer formed on the uppermost surface, it can be used up to high temperatures and can be used at a high temperature.
- a strong optical element can be provided.
- a sixth invention for achieving the above object is the first invention, wherein the environmental resistance is a coefficient of linear expansion.
- a seventh invention for achieving the above object is the first invention, wherein the environmental resistance is moisture resistance.
- moisture resistance As an index of environmental resistance, moisture resistance is used, and by using a resin having high moisture resistance as a resin constituting the resin layer formed on the uppermost surface, even in a high humidity or a high moisture state, Optical elements that are not easily affected can do.
- a first resin layer is formed on a base material, and a second resin layer having a different refractive index from the first resin layer is formed thereon. And, if necessary, a resin layer having a different refractive index from that of the resin layer formed thereunder is sequentially formed thereon, and a predetermined shape is provided at an interface between the resin layers, thereby providing a desired shape.
- An optical element having optical characteristics, and among the resins forming the resin layer, the resin having the largest change in transmittance in a light resistance test using a carbon fade meter is the first resin on the light incident side. It is characterized by not being a layer.
- the resin is denatured and the transmittance is reduced by being exposed to the ultraviolet rays generated from the carbon feed meter.
- the resin is not the first resin layer on the light incident side. Therefore, when receiving ultraviolet rays, the resin having high sensitivity is prevented from receiving ultraviolet rays first, and as a result, an optical element which is strong against ultraviolet rays can be obtained.
- a first resin layer is formed on a base material, and a second resin layer having a different refractive index from the first resin layer is formed thereon. Is formed, and if necessary, a resin layer having a different refractive index from the resin layer formed thereunder is sequentially formed thereon, and the interface between the resin layers is given a predetermined shape.
- the fluorine-containing resin may be a mixture of a plurality of resins or a resin composed of a polymer.
- a tenth invention for achieving the first object is the ninth invention.
- the interface between the fluorine-containing resin and the resin formed thereon is a diffraction optical surface.
- a diffractive optical surface is a surface that produces a diffractive effect on the surface, and generally does not consist of a smooth portion (continuous surface) like a spherical lens or an aspherical lens surface, and has some kind of discontinuity. It has a surface (surface whose surface shape is represented by a discontinuous function).
- a fluorine-containing resin having good releasability from a mold (particularly a mold) and having a diffractive optical surface having a complicated shape such as a relief pattern or a step shape is used.
- the shape can be accurately transferred.
- a first resin layer is formed on a base material having a positive optical power, and a first resin layer and a refractive index of the first resin layer are formed on the first resin layer.
- a different second resin layer is formed, and if necessary, a resin layer formed thereunder and a resin layer having a different refractive index are sequentially formed thereon, and a predetermined layer is formed at an interface between the resin layers.
- An optical element having desired optical characteristics by giving a shape, wherein the refractive index of the first resin layer is smaller than that of the second resin layer, and The interface between the first resin layer and the second resin layer has a relief pattern shape, and the shape of the relief pattern gradually decreases from the center to the periphery of the first resin layer.
- the thickness of the first resin layer is increased, and then the thickness of the first resin layer is increased at a steep gradient.
- a diffractive optical element characterized this' and that but a repeating pattern as decreases.
- the base material has a positive optical power and the first resin A positive optical power is generated by a relief pattern between the layer and the second resin layer.
- the first resin and the mold are separated.
- the portion where the thickness of the first resin layer is reduced is not reduced stepwise but is reduced with a steep gradient.
- the light beam incident on the relief pattern surface is directed to the center of the first resin layer by the positive optical power of the base material.
- the direction of the steep gradient is the same as the direction of this light beam, Rays can be less likely to cross steep interfaces, thereby reducing flare.
- a first resin layer is formed on a base material having a negative optical power, and the first resin layer and the refractive index of the first resin layer are formed on the first resin layer.
- a different second resin layer is formed, and if necessary, a resin layer formed thereunder and a resin layer having a different refractive index are sequentially formed thereon, and a predetermined layer is formed at an interface between the resin layers.
- the interface between the first resin layer and the second resin layer has a relief pattern shape, and the shape of the relief pattern gradually decreases from the center to the periphery of the first resin layer.
- the thickness of the first resin layer decreases, and thereafter, the thickness of the first resin layer decreases at a steep gradient.
- FIG. 1 is a diagram for explaining an example of an embodiment of the present invention.
- FIG. 2 is a diagram for explaining another embodiment of the present invention.
- FIG. 3 is an enlarged schematic view of the diffractive optical surface shown in FIG.
- FIG. 4 is a diagram showing a structure in a case where the diffractive optical element has concave power, and the transparent substrate also has concave power.
- FIG. 5 is an enlarged schematic view of the diffractive optical surface shown in FIG.
- FIG. 6 is a diagram showing an example of a conventional optical element made of a two-layer resin. BEST MODE FOR CARRYING OUT THE INVENTION
- FIG. 1 is a diagram for explaining an example of an embodiment of the present invention, and is a cross-sectional view, but hatching is omitted.
- This optical element has a circular shape when viewed in a plane. These are the same in the following figures.
- a first resin layer 2 is formed on a transparent substrate 1 such as glass as a base material via a silane coupling treatment layer.
- a pattern is formed on the surface of the resin layer 2 so as to give optical characteristics such as a diffraction lens.
- a silane coupling treatment layer is further formed on the first resin layer 2, and a second resin layer 3 having a different refractive index from the first resin layer 2 is formed thereon. Then, a predetermined optical characteristic is obtained by the difference in the refractive index between the first resin layer 2 and the second resin layer 3 and the pattern shape formed between the two.
- FIG. 1 (b) An optical element having the same optical characteristics as the optical element as shown in FIG. 1 (a) can also be realized with a configuration as shown in FIG. 1 (b).
- a first resin layer 3 is formed on a transparent substrate 1 such as glass as a base material via a silane coupling treatment layer.
- a pattern is formed on the surface so as to give optical characteristics such as a diffraction lens.
- a silane coupling layer is further formed on the resin layer 3, and a second resin layer 2 having a different refractive index from the first resin layer 3 is formed thereon. Then, a predetermined optical characteristic is obtained by the difference in the refractive index between the first resin layer 3 and the second resin layer 2 and the pattern shape formed between the two.
- the formation of the silane coupling treatment layer is not always an essential condition.
- the resin layer (resin layer 2 in (a) and resin layer 3 in (b)) sandwiched between the substrate 1 and the uppermost resin layer is exposed directly to the outside air.
- the surface of the uppermost resin layer (resin layer 3 in (a) and resin layer 2 in (b)) is exposed to the outside air.
- the environmental resistance of the resin of the resin layer 2 and the resin of the resin layer 3 are compared, and if the environmental resistance of the resin of the resin layer 2 is superior to the environmental resistance of the resin of the resin layer 3, If the configuration shown in (b) is adopted, and if the environmental resistance of the resin of the resin layer 3 is better than the environmental resistance of the resin of the resin layer 2, the configuration shown in (a) is adopted. Adopt it.
- Indices indicating environmental resistance include, for example, resin hardness, dimensional change due to water absorption, gel fraction, glass transition point, and linear expansion coefficient.
- the resin of the resin layer 2 and the resin of the resin layer 3 are compared with each other in the strength against ultraviolet rays (the resistance to deterioration), and the resin of the resin layer 2 is superior to the resin of the resin layer 3.
- the resin layer 2 in the direction in which light enters, and If the fat is better than the resin of the resin layer 2, the resin layer 3 may be positioned in the direction in which light enters.
- the configuration shown in (a) is adopted, and if the resin of the resin layer 3 is a fluorine-containing resin, the configuration shown in (b) is used.
- FIG. 1 An example of a method for manufacturing an optical element as shown in FIG. 1 will be described below.
- the surface of the transparent substrate 1 is subjected to a silane force pulling process so that a mold having a predetermined shape and the transparent substrate 1 face each other, and a resin layer is interposed between the transparent substrate 1 and the mold using a dispenser or the like. 2 (in the case of Fig. 1 (a)) or resin layer 3 (Fig.
- the resin is filled with an ultraviolet curable resin. Then, ultraviolet rays are irradiated from the transparent substrate 1 side to cure the resin, form a resin layer, and peel the mold. Then, the surface of the formed resin layer is subjected to a silane coupling treatment so that the surface faces a transparent mold having a flat surface, and a resin layer 3 (FIG. 1) is provided between the resin layer and the transparent mold. In the case of (a)) or the resin which forms the resin layer 2 (in the case of FIG. 1 (b)). Then, ultraviolet rays are irradiated from the transparent mold side to cure the filled resin to form a resin layer, and the transparent mold is peeled off.
- FIG. 2 is a diagram for explaining another embodiment of the present invention.
- the transparent substrate 1 may have optical power in addition to the diffractive action on the diffractive optical surface.
- FIG. 2 is a diagram showing a case where the transparent substrate 1 has a positive optical power.
- the optical substrate of the transparent substrate 1 In general, the diffractive optical surface formed at the interface between the two resin layers also has a positive optical power in order to cooperate with the first resin layer.
- 4 is a low refractive index resin layer
- 5 is a high refractive index resin layer.
- the optical element shown in FIG. 2 is manufactured by the same method as the optical element shown in FIG.
- the diffractive optical surface therebetween is as shown in FIG. become.
- the structure is such that the thickness of the high-refractive-index resin layer 5 gradually decreases from the center to the peripheral edge, gradually increases when reaching a certain position, and then gradually decreases from there.
- the diffractive optical surface between them becomes as shown in FIG. Become.
- the thickness of the low-refractive-index resin layer 4 increases smoothly from the center to the periphery, and when the resin layer reaches a certain position, the thickness of the low-refractive-index resin layer 4 gradually decreases, and then the structure gradually increases from there.
- the mold may not be easily peeled off from the resin layer formed between the transparent substrate 1 and the mold. Therefore, the portion corresponding to the step structure is often not a step structure but a portion having a steep gradient. This slope is called draft.
- FIG. 3 is an enlarged schematic view of the diffractive optical surface shown in FIG. Fig. 3 (a) is an enlarged view of the diffractive optical surface (relief pattern surface) between the high refractive index resin layer 5 and the low refractive index resin layer 4 in Fig. 2 (a), and Fig. 3 (b) is FIG. 4B is an enlarged view of the diffractive optical surface (relief pattern surface) between the refractive index resin layer 5 and the low refractive index resin layer 4 in b).
- 6 indicates the draft surface.
- FIG. 3 due to the convex power of the transparent substrate 1 in FIG.
- FIG. 4 is a diagram showing a structure in a case where the diffractive optical element has concave power, and the transparent substrate also has concave power.
- the high refractive index resin layer 5 and the low refractive index resin layer 4 in FIG. 2 may be reversed. Therefore, a high-refractive-index resin layer 5 and a low-refractive-index resin layer 4 are arranged as shown in FIGS. 4 (a) and 4 (b), and the interface between them is shown in FIGS. 4 (a) and 4 (b) This allows the diffractive optical surface to have concave power.
- a resin layer in the case of FIG. 4 (a), a low refractive index resin layer is interposed between the transparent substrate 1 and the mold. 4.
- a draft is provided to improve the peelability.
- FIG. 5 is an enlarged schematic view of the diffractive optical surface shown in FIG. FIG. 5 (a) is an enlarged view of the diffractive optical surface (relief pattern surface) between the high refractive index resin layer 5 and the low refractive index resin layer 4 in FIG. 4 (a), and FIG. 5 (b) is FIG.
- FIG. 3 is an enlarged view of a diffractive optical surface (relief pattern surface) between a high refractive index resin layer 5 and a low refractive index resin layer 4 in FIG.
- 6 indicates the draft surface.
- An optical element having the shape shown in Fig. 1 (a diffraction lens having the function of a convex lens) was formed.
- the outer diameter of the optical element (resin part) is 60 mm in outer diameter
- the diffraction grating is circular
- the pitch is 2 mm near the center of the lens, and as shown in Fig. 1, the pitch becomes narrower toward the outer circumference, and 0.12 in the outer circumference. mm.
- the refractive index of resin 2 is larger than the refractive index of resin 3.
- the properties of the cured products of Resin 2 and Resin 3 are as shown in Table 1.
- Table 1 the change in transmittance before and after the light resistance test using a carbon fade meter (abbreviated as “change in transmittance before and after carbon fume”) is the result of 500 hours of exposure to ultraviolet light emitted from a carbon fade meter device. Things. Glass (BK 7) was used as the substrate 1.
- a diffractive lens with positive power was manufactured.
- the shape of the diffraction grating is as shown in Fig. 2 (b) .
- the outer diameter of the optical element is 60 mm
- the grating height is 20 ⁇
- the grating pitch is 2 mm near the center
- 0.12 mm near the outer periphery. In Thus, the pitch becomes finer toward the outer peripheral surface.
- the high refractive index resin 5 a resin containing urethane acrylate as a main component was used, and as the low refractive index resin 4, a resin containing a fluorinated acrylate was used.
- the relief pattern has a vertical step structure without a draft
- the relief pattern in the second diffractive lens, has a draft as shown in FIG.
- the draft was set such that the gradient increased toward the periphery of the diffraction lens, and the gradient at the outermost circumference was 7 °.
- the low refraction resin 4 was molded using a mold, and the peeling force when the mold was peeled was measured.
- the value of the first diffraction lens was 100 kgf, but the value of the second diffraction lens was reduced to 50 kgf, which was easy to peel.
- the formed grating was observed with a microscope, it was found that the first diffraction lens lacked the grating, whereas the second diffraction lens did not show such a lack of the grating at all. .
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Abstract
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Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2005507268A JPWO2004113971A1 (ja) | 2003-06-19 | 2004-06-17 | 光学素子 |
EP04746291A EP1635197B1 (en) | 2003-06-19 | 2004-06-17 | Optical element |
DE602004030335T DE602004030335D1 (de) | 2003-06-19 | 2004-06-17 | Optisches element |
US11/303,541 US20060182934A9 (en) | 2003-06-19 | 2005-12-16 | Optical element |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2003-174382 | 2003-06-19 | ||
JP2003174382 | 2003-06-19 |
Related Child Applications (1)
Application Number | Title | Priority Date | Filing Date |
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US11/303,541 Continuation-In-Part US20060182934A9 (en) | 2003-06-19 | 2005-12-16 | Optical element |
Publications (1)
Publication Number | Publication Date |
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WO2004113971A1 true WO2004113971A1 (ja) | 2004-12-29 |
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ID=33534789
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Application Number | Title | Priority Date | Filing Date |
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PCT/JP2004/008822 WO2004113971A1 (ja) | 2003-06-19 | 2004-06-17 | 光学素子 |
Country Status (6)
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US (1) | US20060182934A9 (ja) |
EP (1) | EP1635197B1 (ja) |
JP (2) | JPWO2004113971A1 (ja) |
CN (2) | CN101458350A (ja) |
DE (1) | DE602004030335D1 (ja) |
WO (1) | WO2004113971A1 (ja) |
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US20060093793A1 (en) | 2006-05-04 |
EP1635197A4 (en) | 2007-10-10 |
CN101458350A (zh) | 2009-06-17 |
DE602004030335D1 (de) | 2011-01-13 |
JPWO2004113971A1 (ja) | 2006-08-03 |
CN100514091C (zh) | 2009-07-15 |
CN1809769A (zh) | 2006-07-26 |
US20060182934A9 (en) | 2006-08-17 |
EP1635197A1 (en) | 2006-03-15 |
JP5045739B2 (ja) | 2012-10-10 |
EP1635197B1 (en) | 2010-12-01 |
JP2010102353A (ja) | 2010-05-06 |
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