JPH0957771A - Method for manufacturing composite optical element - Google Patents
Method for manufacturing composite optical elementInfo
- Publication number
- JPH0957771A JPH0957771A JP21496995A JP21496995A JPH0957771A JP H0957771 A JPH0957771 A JP H0957771A JP 21496995 A JP21496995 A JP 21496995A JP 21496995 A JP21496995 A JP 21496995A JP H0957771 A JPH0957771 A JP H0957771A
- Authority
- JP
- Japan
- Prior art keywords
- resin layer
- optical element
- mold
- base material
- resin
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Landscapes
- Moulds For Moulding Plastics Or The Like (AREA)
- Casting Or Compression Moulding Of Plastics Or The Like (AREA)
Abstract
(57)【要約】
【課題】 直径の小さな複合型光学素子を製造する。
【解決手段】 光学素子基材成形面にエネルギー硬化型
の樹脂を供給し、金型と光学素子基材とを相対的に接近
させることにより前記樹脂を押し広げて金型と光学素子
基材との間に所望の樹脂層を形成した後、エネルギーの
照射により樹脂層を硬化させ、その後に硬化した樹脂層
と金型とを剥離する複合型光学素子の製造方法にあっ
て、形成する樹脂層3のうち光学性能に関係のある部分
を光学素子基材2の中心軸に対して非軸対称形状とし、
光学素子基材2の中心軸上の点を中心とする樹脂層3の
有効直径の最大値を直径とした円内における光学性能に
無関係な光学素子基材2の部分に荷重を加えて金型と硬
化した樹脂層3との剥離を行い、前記有効直径の外側に
剥離用の荷重を加える基材部分を不要にする。
(57) Abstract: A composite optical element having a small diameter is manufactured. An energy-curable resin is supplied to a molding surface of an optical element base material, and the mold and the optical element base material are relatively brought close to each other to spread the resin to spread the mold and the optical element base material. In the method of manufacturing a composite optical element, the resin layer is formed by curing a resin layer by irradiating energy after a desired resin layer is formed between A portion of 3 which is related to optical performance is formed in a non-axisymmetric shape with respect to the central axis of the optical element substrate 2,
A mold is formed by applying a load to a portion of the optical element substrate 2 which is irrelevant to the optical performance within a circle whose diameter is the maximum effective diameter of the resin layer 3 centered on a point on the central axis of the optical element substrate 2. And the cured resin layer 3 are peeled off, and the base material portion for applying a peeling load to the outside of the effective diameter is unnecessary.
Description
【0001】[0001]
【発明の属する技術分野】本発明は、光学素子基材上に
樹脂層を載置した複合型光学素子の製造方法に関する。The present invention relates to a method for manufacturing a composite optical element in which a resin layer is mounted on an optical element substrate.
【0002】[0002]
【従来の技術】従来技術としては、特開平4−1447
18号公報がある。この方法は、金型と硬化した樹脂層
を剥離する時に、樹脂層表面の光学性能に関係のない部
分(有効直径外の部分)に荷重を加えることにより、金
型と樹脂層の容易な剥離を実現するものであるが、樹脂
層の光学性能に関係のある部分(有効直径内の部分)の
形状は中心軸対称形状となっている。2. Description of the Related Art As the prior art, Japanese Patent Laid-Open No. 4-1447
There is a publication No. 18. In this method, when the mold and the cured resin layer are peeled off, a load is applied to the part of the resin layer surface that is not related to the optical performance (the part outside the effective diameter), so that the mold and the resin layer can be easily separated. However, the shape of the portion related to the optical performance of the resin layer (the portion within the effective diameter) is symmetrical about the central axis.
【0003】[0003]
【発明が解決しようとする課題】しかし、前記従来技術
の方法では、金型と硬化した樹脂層を剥離する時に、樹
脂層の光学性能に関係のない部分に荷重を加えているの
で、複合型光学素子の直径を有効直径に対してある程度
大きくする必要がある。荷重を加える部分が狭いと、半
径方向において部分的に応力が集中するので、有効直径
内の樹脂部が有効直径外の樹脂部の変形の影響を受け
て、樹脂層表面が所望の光学面形状にならないという問
題が発生する。また、光学素子基材が破損するという問
題も同時に発生する場合がある。However, in the method of the prior art described above, when the mold and the cured resin layer are peeled off, a load is applied to a portion of the resin layer that is not related to the optical performance. It is necessary to make the diameter of the optical element larger than the effective diameter to some extent. If the part to which the load is applied is narrow, the stress will be concentrated in the radial direction, so the resin part within the effective diameter will be affected by the deformation of the resin part outside the effective diameter, and the resin layer surface will have the desired optical surface shape. There is a problem that it does not become. In addition, the problem that the optical element substrate is damaged may occur at the same time.
【0004】そこで、荷重を加える部分の幅を広くする
と、必然的に複合型光学素子自体の直径も大きくなる。
当然のことながら、ここで製造した複合型光学素子を用
いる製品も大きくなる。Therefore, if the width of the portion to which the load is applied is increased, the diameter of the composite optical element itself is inevitably increased.
As a matter of course, the product using the composite optical element manufactured here also becomes large.
【0005】しかし、カメラ等の分野では製品の小型化
の競争が激しく、性能に直接関係のない部分が増えるこ
とは望ましくない。特に、小さくすること自体がメリッ
トの一つであるコンパクトカメラのような製品では、魅
力が著しく損なわれるという致命的な問題となる。However, in the field of cameras and the like, there is intense competition for product miniaturization, and it is not desirable to increase the number of parts that are not directly related to performance. In particular, in a product such as a compact camera, in which miniaturization itself is one of the merits, it is a fatal problem that attractiveness is significantly impaired.
【0006】本発明は、上記従来技術の問題点に鑑みて
なされたもので、光学性能に関係する樹脂層の有効直径
よりも外側に、金型と硬化した樹脂層を剥離する時に荷
重を加えるための部分を設ける必要がない、直径の小さ
な複合型光学素子を製造することができる複合型光学素
子の製造方法を提供することを目的とする。The present invention has been made in view of the above problems of the prior art, and a load is applied to the outside of the effective diameter of the resin layer related to the optical performance when the mold and the cured resin layer are peeled off. It is an object of the present invention to provide a method for manufacturing a composite optical element, which can manufacture a composite optical element having a small diameter without the need to provide a portion for.
【0007】[0007]
【課題を解決するための手段】上記課題を解決するため
に、本発明は以下のように構成した。請求項1の発明
は、光学素子基材成形面にエネルギー硬化型の樹脂を供
給し、金型と光学素子基材とを相対的に接近させること
により前記樹脂を押し広げて金型と光学素子基材との間
に所望の樹脂層を形成した後、エネルギーの照射により
樹脂層を硬化させ、その後に硬化した樹脂層と金型とを
剥離する複合型光学素子の製造方法において、形成する
樹脂層のうち光学性能に関係のある部分を光学素子基材
成形面の中心軸に対して非軸対称形状とし、かつ光学素
子基材成形面の中心軸上の点を中心とする樹脂層の有効
直径の最大値を直径とした円内における光学性能に無関
係な部分に荷重を加え、金型と硬化した樹脂層との剥離
を行うこととした。Means for Solving the Problems In order to solve the above problems, the present invention is configured as follows. According to a first aspect of the present invention, an energy-curable resin is supplied to the molding surface of the optical element base material, and the mold and the optical element base material are relatively brought close to each other to spread the resin to spread the resin and the mold. After forming a desired resin layer between the substrate and the substrate, the resin layer is cured by irradiation with energy, and the resin is formed in the method for producing a composite optical element in which the cured resin layer and the mold are separated. The part of the layer that is related to optical performance is made non-axisymmetric with respect to the central axis of the optical element substrate molding surface, and the resin layer centered on a point on the central axis of the optical element substrate molding surface is effective It was decided to apply a load to a portion having no relation to the optical performance within a circle having the maximum value of the diameter as a diameter, and to separate the mold from the cured resin layer.
【0008】請求項2の発明は、請求項1の構成にあっ
て、光学性能に無関係な部分が樹脂層であるようにし
た。According to a second aspect of the present invention, in the structure of the first aspect, the portion unrelated to the optical performance is the resin layer.
【0009】請求項3の発明は、請求項1の構成にあっ
て、光学性能に無関係な部分が光学素子基材であるよう
にした。。According to a third aspect of the present invention, in the structure of the first aspect, the portion unrelated to the optical performance is the optical element substrate. .
【0010】請求項1の作用を説明する。現在、一般に
使用されているフィルムは長方形なので、フィルム面に
届く光線は必ずしも光学素子基材の中心軸を中心とする
軸対称形状である必要はない。したがって、複合型光学
素子の光学性能に関係がある有効直径自体も必ずしも軸
対称形状である必要はない。The operation of claim 1 will be described. Currently used films are generally rectangular, so that the light rays that reach the film surface do not necessarily have to be axisymmetrical about the central axis of the optical element substrate. Therefore, the effective diameter itself, which is related to the optical performance of the composite optical element, does not necessarily have to be axisymmetric.
【0011】しかし、複合型光学素子の基材としてはガ
ラスが用いられることが多いが、ガラスは軸対称形状に
加工するよりも非軸対称形状に加工する方がコストがか
かる。また、複合型光学素子の製造では基材上に載置し
た樹脂を金型で押圧して樹脂層を形成するので、前記基
材が非軸対称形状の場合は、製造時の位置決め等の作業
において動作数が増えるため好ましくない。これに対
し、基材上に載置する樹脂層はある程度自由な形状とす
ることが可能である。樹脂層を形成する金型は一旦製作
すれば長期間使用できるので、基材を非軸対称形状に加
工する場合に比べるとコストはほとんど無視できる。However, although glass is often used as the base material of the composite optical element, it is more costly to process glass into a non-axisymmetric shape than to process it into an axisymmetric shape. Further, in manufacturing a composite type optical element, a resin placed on a base material is pressed by a mold to form a resin layer. Therefore, when the base material has a non-axisymmetric shape, work such as positioning during manufacturing is performed. Is not preferable because the number of operations increases. On the other hand, the resin layer mounted on the base material can be formed to have a free shape to some extent. Since the mold for forming the resin layer can be used for a long time once manufactured, the cost can be almost ignored as compared with the case where the base material is processed into a non-axisymmetric shape.
【0012】そこで、中心軸対称形状の基材上に、光学
性能に関係のある部分が非軸対称形状の樹脂層を載置す
れば、金型と硬化した樹脂層を剥離する時に光学性能に
無関係な部分に荷重をかけることにより、従来技術と同
様な手段で金型と樹脂層の容易な剥離が実現可能とな
る。Therefore, by placing a resin layer having a non-axisymmetric portion in relation to the optical performance on a substrate having a central axis symmetrical shape, the optical performance is improved when the mold and the cured resin layer are peeled off. By applying a load to an irrelevant portion, it becomes possible to easily separate the mold and the resin layer by the same means as in the conventional technique.
【0013】そして、請求項2の構成にあっては、樹脂
層自体を軸対称形状とし、樹脂層の光学性能に関係のあ
る部分を非軸対称形状にすることで、樹脂層の硬化が完
了した直後に、まずは樹脂層の光学性能に無関係な部分
において金型と樹脂層を剥離し、次に金型を剥離した樹
脂層に荷重を加えて金型と複合型光学素子との剥離がな
される。According to the second aspect of the invention, the resin layer itself is formed in an axially symmetric shape, and the portion of the resin layer that is related to the optical performance is formed in a non-axisymmetrical shape, whereby the curing of the resin layer is completed. Immediately after that, the mold and the resin layer are first peeled off at a portion unrelated to the optical performance of the resin layer, and then the mold and the composite optical element are peeled off by applying a load to the resin layer after peeling the mold. It
【0014】また、請求項3の構成にあっては、樹脂層
自体を非軸対称形状とし、樹脂層の硬化が完了した後に
そのまま基材上の樹脂層を形成していない部分に荷重を
加えて金型と複合型光学素子との剥離がなされる。According to the third aspect of the present invention, the resin layer itself has a non-axisymmetric shape, and a load is applied to the portion of the base material on which the resin layer is not formed after the resin layer is completely cured. And the composite optical element is peeled off.
【0015】[0015]
[発明の実施の形態1]本発明の実施の形態1を図1〜
図10に基づいて説明する。図1に示すように、両面が
凹面のガラス製の光学素子基材(以下、基材という)2
に樹脂5が必要量吐出されている。基材2の成形面(樹
脂層を載置する面)の曲率半径は100mm、非成形面
(樹脂層を載置しない面)の曲率半径は80mm、外径
は25mmである。また、樹脂5の必要量は予め求めら
れているものとする。[First Embodiment of the Invention] FIG.
A description will be given based on FIG. As shown in FIG. 1, a glass optical element substrate (hereinafter, referred to as substrate) 2 having concave surfaces on both sides 2
The required amount of resin 5 has been discharged to. The radius of curvature of the molding surface (the surface on which the resin layer is placed) of the base material 2 is 100 mm, and the radius of curvature of the non-molding surface (the surface on which the resin layer is not mounted) is 80 mm and the outer diameter is 25 mm. Also, the required amount of the resin 5 is assumed to be obtained in advance.
【0016】一方、本実施の形態に用いる金型1は、基
材2上に所望の樹脂層表面を形成するための光学面(樹
脂層を押圧する面)1aを有し、かつ中心軸が基材2の
中心軸と同一で上下動自在に保持されている。金型1の
光学面1aの外周部の形状(輪郭)は非軸対称形状をし
ており、金型1の光学面1aの中心軸上の点を原点とし
て中心軸に垂直なxy平面上に、金型1の光学面1aの
外周部の各点を中心軸に平行に移動させると、図2に示
すようにx軸に対して上下50度の範囲は直径25mm
の円弧1b形状で、その他の部分は2つの円弧1bの端
点を結ぶy座標が一定の直線1c形状である。On the other hand, the mold 1 used in this embodiment has an optical surface (a surface for pressing the resin layer) 1a for forming a desired resin layer surface on the base material 2 and has a central axis. It is held in the same manner as the central axis of the base material 2 so as to be vertically movable. The shape (outline) of the outer peripheral portion of the optical surface 1a of the mold 1 is a non-axisymmetric shape, and the point on the central axis of the optical surface 1a of the mold 1 is the origin and is on the xy plane perpendicular to the central axis. When each point on the outer peripheral portion of the optical surface 1a of the mold 1 is moved in parallel with the central axis, a range of 50 degrees up and down with respect to the x axis is 25 mm in diameter as shown in FIG.
The shape is a circular arc 1b, and the other portion is a straight line 1c having a constant y coordinate connecting the end points of the two circular arcs 1b.
【0017】次に、金型1を下降して基材2に近づける
ことにより、光学面1aで樹脂5を広げて所望の厚さの
樹脂層3を形成する工程を説明する。基材2上に形成す
る樹脂層3の光学性能に関係のある部分は、x軸に対し
て上下45度の範囲が直径24mmの円弧で、その他の
部分が2つの端点を結ぶy座標が一定の直線で囲まれた
領域である。金型1を下降して樹脂5を押圧すると、樹
脂5が金型1の光学面1aの外周部からはみ出す直前ま
では、図3(x軸方向から見た中心軸を含む断面図)お
よび図4(y軸方向から見た中心軸を含む断面図)に示
すように、樹脂5は基材2上で同心円状に広がる。そし
て、さらに金型1を下降すると、樹脂5が金型1の光学
面1aの直線1c形状部分からはみ出す。樹脂5が金型
1の光学面1aの外周部からはみ出すと(はみ出した部
分の表面を5aとする)、まだ押圧されている樹脂5と
それ以外では樹脂5が半径方向に広がる速度が異なり、
図5(x軸方向から見た中心軸を含む断面図)および図
6(y方向から見た中心軸を含む断面図)に示すよう
に、基材2上の樹脂5の形状は同心円状ではなくなる。
すなわち、樹脂5の金型1の光学面1aの外周部からは
み出した部分5aは金型1を下降させることによる圧力
を受けないので、半径方向にはほとんど広がらず、垂直
方向に広がるためである。そして、中心軸上の樹脂層3
が所望の厚さになる時点まで金型1を下降し、所望の樹
脂層3を形成する。この時、図7に示すように前記光学
性能に関係のある領域全体に樹脂5が押し広げられるよ
うに、予め基材2上に吐出する樹脂5の量を調整してお
く必要がある。なお、図7は樹脂層3を中心軸に平行な
方向から基板2の方向を見た平面図である。Next, a process of forming the resin layer 3 having a desired thickness by spreading the resin 5 on the optical surface 1a by lowering the mold 1 and bringing it closer to the base material 2 will be described. The part related to the optical performance of the resin layer 3 formed on the base material 2 is an arc having a diameter of 24 mm in the range of 45 degrees up and down with respect to the x axis, and the other parts have a constant y coordinate connecting the two end points. The area surrounded by the straight line. When the mold 1 is lowered and the resin 5 is pressed, the resin 5 is shown in FIG. 3 (a cross-sectional view including the central axis viewed from the x-axis direction) until immediately before the resin 5 protrudes from the outer peripheral portion of the optical surface 1 a of the mold 1. As shown in FIG. 4 (cross-sectional view including the central axis when viewed from the y-axis direction), the resin 5 spreads concentrically on the base material 2. Then, when the mold 1 is further lowered, the resin 5 protrudes from the straight line 1c shaped portion of the optical surface 1a of the mold 1. When the resin 5 protrudes from the outer peripheral portion of the optical surface 1a of the mold 1 (the surface of the protruding portion is referred to as 5a), the speed at which the resin 5 spreads in the radial direction differs between the resin 5 which is still pressed and the other portions,
As shown in FIG. 5 (cross-sectional view including the central axis viewed from the x-axis direction) and FIG. 6 (cross-sectional view including the central axis viewed from the y-direction), the shape of the resin 5 on the base material 2 is concentric. Disappear.
That is, the portion 5a of the resin 5 protruding from the outer peripheral portion of the optical surface 1a of the mold 1 is not subjected to the pressure caused by the lowering of the mold 1, so that it does not spread in the radial direction but spreads in the vertical direction. . And the resin layer 3 on the central axis
The mold 1 is lowered to a desired thickness to form the desired resin layer 3. At this time, as shown in FIG. 7, it is necessary to previously adjust the amount of the resin 5 discharged onto the base material 2 so that the resin 5 is spread over the entire region related to the optical performance. Note that FIG. 7 is a plan view of the resin layer 3 as seen from the direction parallel to the central axis of the substrate 2.
【0018】次に、この状態で基材2の下方から不図示
の手段により紫外線を照射し、樹脂層3を硬化する。そ
して、エネルギーの照射が完了した時点では金型1、基
材2および硬化した樹脂層3が一体となった密着体が形
成されている。Next, in this state, ultraviolet rays are irradiated from below the base material 2 by means not shown to cure the resin layer 3. Then, when the irradiation of energy is completed, a close contact body in which the mold 1, the base material 2 and the cured resin layer 3 are integrated is formed.
【0019】次に、図8に示すように、前記密着体を上
昇させると、基材2の樹脂層3を形成していない部分の
上方に予め設けられていた剥離用の部材4が基材2の表
面2aと接触する。すると、基材2の表面2a上の剥離
用の部材4が接触した部分にまず荷重が集中し、その後
荷重が基材2の全体に分散する。そして、このまま前記
密着体の上昇を続けると、図9に示すように金型1から
樹脂層3が剥離し、基材2と樹脂層3が一体となった複
合型光学素子6が得られる。図10に製造した複合型光
学素子6を上から見た図を示す。Next, as shown in FIG. 8, when the contact member is raised, the peeling member 4 previously provided above the portion of the base material 2 on which the resin layer 3 is not formed is removed. It comes into contact with the surface 2a of the second. Then, the load is first concentrated on the portion on the surface 2a of the base material 2 where the peeling member 4 is in contact, and then the load is dispersed over the entire base material 2. Then, if the contact body is continuously raised as it is, the resin layer 3 is separated from the mold 1 as shown in FIG. 9, and the composite optical element 6 in which the base material 2 and the resin layer 3 are integrated is obtained. FIG. 10 shows a view of the manufactured composite optical element 6 as seen from above.
【0020】本発明の実施の形態の製造方法によると、
基材2を最大有効直径よりも僅かに大きくしただけで、
金型1と硬化した樹脂層3の容易な剥離を実現すること
ができる。According to the manufacturing method of the embodiment of the present invention,
By making the base material 2 slightly larger than the maximum effective diameter,
The mold 1 and the cured resin layer 3 can be easily peeled off.
【0021】[発明の実施の形態2]本発明の実施の形
態2を図11〜図15に基づいて説明する。図11に示
すように、両面が凹面のガラス製の基材12に樹脂15
が必要量吐出されている。基材12の成形面(樹脂層を
載置する面)の曲率半径は100mm、非成形面(樹脂
層を載置しない面)の曲率半径は80mm、外径は42
mmである。また、樹脂15の必要量は予め求められて
いるものとする。[Second Embodiment of the Invention] A second embodiment of the present invention will be described with reference to FIGS. As shown in FIG. 11, resin 15 is applied to the glass substrate 12 having concave surfaces on both sides.
Is being discharged in the required amount. The radius of curvature of the molding surface (the surface on which the resin layer is placed) of the base material 12 is 100 mm, the radius of curvature of the non-molding surface (the surface on which the resin layer is not mounted) is 80 mm, and the outer diameter is 42.
mm. The required amount of the resin 15 is assumed to be obtained in advance.
【0022】一方、本実施の形態に用いる金型11は、
図13および図14に示すように、軸方向へ相対的に移
動可能なA型11aとB型11bを組み合わせて構成さ
れ、A型11aとB型11bの端面を段差のない状態に
して樹脂15を押圧する型光学面に形成し、直径42m
mの軸対称形状となっている。すなわち、金型11の型
光学面の中心軸上の点を原点として、中心軸をz軸、こ
の中心軸に垂直で、かつ互いに垂直な方向にx,y軸を
設定すると、図12に示すように、x軸からの距離が1
9mmの位置で光学性能に関係のある部分を含めて押圧
するA型11aと光学性能に無関係な部分のみを押圧す
るB型11bの互いに上下動自在な2部品に分割されて
おり、A型11a、B型11bともに所望の樹脂層表面
を形成するための光学面を有し、かつ金型11の中心軸
は基材12の中心軸と同一になっている。On the other hand, the mold 11 used in this embodiment is
As shown in FIGS. 13 and 14, the A type 11a and the B type 11b, which are relatively movable in the axial direction, are combined, and the end faces of the A type 11a and the B type 11b are made to have no step and the resin 15 is formed. Formed on the optical surface of the mold that presses, with a diameter of 42 m
It has an axisymmetric shape of m. That is, when a point on the center axis of the mold optical surface of the mold 11 is the origin, the center axis is the z axis, and the x and y axes are set in the directions perpendicular to the center axis and mutually perpendicular, the result is shown in FIG. So the distance from the x-axis is 1
It is divided into two vertically movable parts, an A type 11a that presses at a position of 9 mm including a part related to optical performance and a B type 11b that presses only a part unrelated to optical performance. , B mold 11b both have an optical surface for forming a desired resin layer surface, and the central axis of the mold 11 is the same as the central axis of the base material 12.
【0023】次に、複合型光学素子の製造方法を説明す
る。まず、図13に示すように、A型11aの光学面と
B型11bの光学面の境界において段差がない状態で、
金型11を下降して基材12に近づけることにより基材
12上で樹脂15を押し広げ、所望の厚さの樹脂層13
を形成する位置で金型11の下降を停止する。Next, a method for manufacturing the composite optical element will be described. First, as shown in FIG. 13, in the state where there is no step at the boundary between the optical surface of the A type 11a and the optical surface of the B type 11b,
The resin 15 is spread on the base material 12 by lowering the mold 11 and bringing it closer to the base material 12 to form a resin layer 13 having a desired thickness.
The lowering of the mold 11 is stopped at the position where the mold is formed.
【0024】次に、この状態で基材12の下方から不図
示の手段により紫外線を照射し、樹脂層13を硬化す
る。そして、エネルギーの照射が完了した時点では金型
11、基材12および硬化した樹脂層13が一体となっ
た密着体が形成されている。Next, in this state, ultraviolet rays are irradiated from below the base material 12 by means not shown to cure the resin layer 13. Then, when the irradiation of energy is completed, a contact body in which the mold 11, the base material 12, and the cured resin layer 13 are integrated is formed.
【0025】次に、図14に示すように、B型11bを
上昇し、光学性能に無関係な部分のB型11bを前記密
着体から剥離する。この時、B型11bが樹脂層13と
密着している光学面の面積は、A型11aが樹脂層13
と密着している光学面の面積に比べて少なく、A型11
aと樹脂層13は互いに固定されているので、B型11
bは樹脂層13の表面13aから容易に剥離できる。そ
して、B型11bを樹脂層13表面から剥離した後に、
予め基材12の有効直径よりも外側に設けられていた剥
離用の部材14を、B型11bを剥離した部分の樹脂層
13の表面13a上方に移動させる。Next, as shown in FIG. 14, the B mold 11b is raised and the part of the B mold 11b irrelevant to the optical performance is peeled off from the contact body. At this time, the area of the optical surface where the B type 11b is in close contact with the resin layer 13 is the same as that of the A type 11a.
It is smaller than the area of the optical surface that is in close contact with
Since a and the resin layer 13 are fixed to each other, the B type 11
b can be easily peeled off from the surface 13a of the resin layer 13. Then, after peeling the B type 11b from the surface of the resin layer 13,
The peeling member 14, which is provided outside the effective diameter of the base material 12 in advance, is moved above the surface 13a of the resin layer 13 in the portion where the B mold 11b is peeled off.
【0026】次に、A型11aと樹脂層13と基材12
の密着体を上昇させると、剥離用の部材14が樹脂層1
3の表面13aと接触し、まず樹脂層13の表面13a
上の剥離用の部材14が接触した部分に荷重が集中し、
その後に荷重が樹脂層13から基材12の全体に分散す
る。そして、このまま前記密着体の上昇を続けると、図
15に示すように、A型11aから基材12と樹脂層1
3が一体となった複合型光学素子16が剥離される。製
造した複合型光学素子16の樹脂層13の表面13aに
は、金型11の型光学面を形成するA型11aの光学面
とB型11bの光学面による境界線の跡や、剥離用の部
材14で押圧した跡が残るが、この部分は光学性能に関
係のない部分なので、性能上全く問題はない。Next, the A type 11a, the resin layer 13 and the substrate 12
When the adhered body of is lifted, the peeling member 14 becomes the resin layer 1
The surface 13a of the resin layer 13 is first contacted with the surface 13a of
The load is concentrated on the portion where the upper peeling member 14 is in contact,
After that, the load is dispersed from the resin layer 13 to the entire substrate 12. Then, if the above-mentioned close contact is continuously raised as it is, as shown in FIG. 15, from the A type 11a to the base material 12 and the resin layer 1.
The composite optical element 16 in which 3 is integrated is peeled off. On the surface 13a of the resin layer 13 of the manufactured composite optical element 16, there are traces of a boundary line between the optical surfaces of the A-type 11a and the B-type 11b forming the mold optical surface of the mold 11, and peeling. Although a trace of pressing by the member 14 remains, this portion has no relation to the optical performance, so there is no problem in terms of performance.
【0027】本発明の実施の形態の製造方法によると、
基材12を最大有効直径よりも僅かに大きくしただけ
で、金型11と硬化した樹脂層13の容易な剥離を実現
することができる。According to the manufacturing method of the embodiment of the present invention,
Only by making the base material 12 slightly larger than the maximum effective diameter, the mold 11 and the cured resin layer 13 can be easily peeled off.
【0028】[0028]
【発明の効果】以上のように、本発明の請求項1〜3に
係る複合型光学素子の製造方法によれば、光学素子基材
を樹脂層の光学性能に関係する最大有効直径よりも僅か
に大きくしただけで、金型と硬化した樹脂層の容易な剥
離を実現することができ、製品の小型化の要求に対応し
得る複合型光学素子を製造することができる。As described above, according to the method for manufacturing a composite optical element according to claims 1 to 3 of the present invention, the optical element substrate is made smaller than the maximum effective diameter related to the optical performance of the resin layer. By simply increasing the size, the mold and the cured resin layer can be easily peeled off, and a composite optical element that can meet the demand for downsizing of the product can be manufactured.
【図1】本発明の実施の形態1の一工程を示す断面図
で、基材上に樹脂を吐出した状態を示している。FIG. 1 is a cross-sectional view showing a step of a first embodiment of the present invention, showing a state where a resin is discharged onto a base material.
【図2】本発明の実施の形態1に用いる金型の光学面を
示す平面図である。FIG. 2 is a plan view showing an optical surface of a mold used in the first embodiment of the present invention.
【図3】本発明の実施の形態1の一工程を示す断面図
で、図2のx軸の方向から見た図である。FIG. 3 is a cross-sectional view showing a step of the first embodiment of the present invention, as seen from the direction of the x-axis in FIG.
【図4】本発明の実施の形態1の一工程を示す断面図
で、図2のy軸の方向から見た図である。FIG. 4 is a cross-sectional view showing a step of the first embodiment of the present invention, as seen from the direction of the y-axis in FIG.
【図5】本発明の実施の形態1の一工程を示す断面図
で、図2のx軸の方向から見た図である。5 is a cross-sectional view showing a step of the first embodiment of the present invention, as seen from the direction of the x-axis in FIG. 2. FIG.
【図6】本発明の実施の形態1の一工程を示す断面図
で、図2のy軸の方向から見た図である。FIG. 6 is a cross-sectional view showing a step of the first embodiment of the present invention, as seen from the direction of the y-axis in FIG.
【図7】本発明の実施の形態1により基材上に形成する
樹脂層を示す平面図である。FIG. 7 is a plan view showing a resin layer formed on a base material according to the first embodiment of the present invention.
【図8】本発明の実施の形態1の一工程を示す断面図
で、樹脂層と金型を剥離する状態を示している。FIG. 8 is a cross-sectional view showing a step of the first embodiment of the present invention, showing a state where the resin layer and the mold are peeled off.
【図9】本発明の実施の形態1の一工程を示す断面図
で、金型と複合型光学素子を剥離した状態を示してい
る。FIG. 9 is a cross-sectional view showing a step of the first embodiment of the present invention, showing a state where the mold and the composite optical element are separated.
【図10】本発明の実施の形態1により製造した複合型
光学素子を示す平面図である。FIG. 10 is a plan view showing a composite optical element manufactured according to the first embodiment of the present invention.
【図11】本発明の実施の形態2の一工程を示す断面図
で、基材上に樹脂を吐出した状態を示している。FIG. 11 is a cross-sectional view showing a step of the second embodiment of the present invention, showing a state where resin is discharged onto the base material.
【図12】本発明の実施の形態2に用いる金型の光学面
を示す平面図である。FIG. 12 is a plan view showing an optical surface of a mold used in Embodiment 2 of the present invention.
【図13】本発明の実施の形態2の一工程を示す断面図
で、樹脂層を形成した状態を示している。FIG. 13 is a cross-sectional view showing a step of the second embodiment of the present invention, showing a state in which a resin layer has been formed.
【図14】本発明の実施の形態2の一工程を示す断面図
で、一方の金型を樹脂から剥離した状態を示している。FIG. 14 is a cross-sectional view showing a step of the second embodiment of the present invention, showing a state where one mold is separated from the resin.
【図15】本発明の実施の形態2の一工程を示す断面図
で、金型と複合型光学素子を剥離した状態を示してい
る。FIG. 15 is a cross-sectional view showing a step of the second embodiment of the present invention, showing a state where the mold and the composite optical element are separated.
1,11 金型 2,12 光学素子基材 3,13 樹脂層 4,14 剥離用の部材 5,15 樹脂 6,16 複合型光学素子 DESCRIPTION OF SYMBOLS 1,11 Mold 2,12 Optical element base material 3,13 Resin layer 4,14 Separation member 5,15 Resin 6,16 Composite type optical element
Claims (3)
の樹脂を供給し、金型と光学素子基材とを相対的に接近
させることにより前記樹脂を押し広げて金型と光学素子
基材との間に所望の樹脂層を形成した後、エネルギーの
照射により樹脂層を硬化させ、その後に硬化した樹脂層
と金型とを剥離する複合型光学素子の製造方法におい
て、形成する樹脂層のうち光学性能に関係のある部分を
光学素子基材成形面の中心軸に対して非軸対称形状と
し、かつ光学素子基材成形面の中心軸上の点を中心とす
る樹脂層の有効直径の最大値を直径とした円内における
光学性能に無関係な部分に荷重を加え、金型と硬化した
樹脂層との剥離を行うことを特徴とする複合型光学素子
の製造方法。1. An energy-curable resin is supplied to a molding surface of an optical element base material, and the mold and the optical element base material are relatively brought close to each other to spread the resin to spread the mold and the optical element base material. After forming a desired resin layer between and, the resin layer is cured by irradiation with energy, and then the cured resin layer and the mold are separated, Of the effective diameter of the resin layer centered on a point on the central axis of the optical element substrate molding surface, the portion related to optical performance is made non-axisymmetric with respect to the central axis of the optical element substrate molding surface. A method for producing a composite-type optical element, characterized in that a load is applied to a portion having no relation to optical performance within a circle having a maximum value as a diameter to separate the mold from the cured resin layer.
あることを特徴とする請求項1記載の複合型光学素子の
製造方法。2. The method for producing a composite optical element according to claim 1, wherein the portion unrelated to the optical performance is a resin layer.
基材であることを特徴とする請求項1記載の複合型光学
素子の製造方法。3. The method for producing a composite optical element according to claim 1, wherein the portion unrelated to the optical performance is an optical element base material.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP21496995A JP3544587B2 (en) | 1995-08-23 | 1995-08-23 | Method for manufacturing composite optical element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP21496995A JP3544587B2 (en) | 1995-08-23 | 1995-08-23 | Method for manufacturing composite optical element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0957771A true JPH0957771A (en) | 1997-03-04 |
| JP3544587B2 JP3544587B2 (en) | 2004-07-21 |
Family
ID=16664561
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP21496995A Expired - Fee Related JP3544587B2 (en) | 1995-08-23 | 1995-08-23 | Method for manufacturing composite optical element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3544587B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2003094460A (en) * | 2001-09-27 | 2003-04-03 | Nikon Corp | Method and apparatus for manufacturing resin-bonded optical element |
-
1995
- 1995-08-23 JP JP21496995A patent/JP3544587B2/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2003094460A (en) * | 2001-09-27 | 2003-04-03 | Nikon Corp | Method and apparatus for manufacturing resin-bonded optical element |
Also Published As
| Publication number | Publication date |
|---|---|
| JP3544587B2 (en) | 2004-07-21 |
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