JPH01312505A - Mirror and production thereof - Google Patents

Mirror and production thereof

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Publication number
JPH01312505A
JPH01312505A JP14289488A JP14289488A JPH01312505A JP H01312505 A JPH01312505 A JP H01312505A JP 14289488 A JP14289488 A JP 14289488A JP 14289488 A JP14289488 A JP 14289488A JP H01312505 A JPH01312505 A JP H01312505A
Authority
JP
Japan
Prior art keywords
mirror
electrostrictive element
electric field
reflective film
film
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.)
Pending
Application number
JP14289488A
Other languages
Japanese (ja)
Inventor
Yoichi Hashimoto
陽一 橋本
Osamu Hamada
治 浜田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP14289488A priority Critical patent/JPH01312505A/en
Publication of JPH01312505A publication Critical patent/JPH01312505A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、例えば切断・溶接等に用いるレーザ加工機や
レーザディスク、コンパクトディスク等の電子機器など
のミラーとして広く利用できる、電気的にリアルタイム
で光軸を変化させることが可能なミラー、及びその製造
方法に関するものである。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention is an electrical real-time system that can be widely used as a mirror in laser processing machines used for cutting and welding, laser discs, compact discs, and other electronic devices. The present invention relates to a mirror whose optical axis can be changed in a single direction, and a method for manufacturing the mirror.

[従来の技術] 第5図は、例えばレーザ応用技術ハンドブック(レーザ
協会編集、朝倉書店、1984年発行)の56〜57頁
に示されている従来の光学素子を用いた場合の光軸と曲
率半径との関係を示す特性図である。図に示すように、
鏡の曲率半径がbl、b2、両者の間隔がdの共賑器で
、一方の鏡がθだけ回転したとすると、ミラーの曲率中
心を結ぶ線は角度φ回転する。角度がちいさいときには
次式が成立する。
[Prior art] Figure 5 shows the optical axis and curvature when a conventional optical element is used, for example, as shown on pages 56-57 of the Laser Application Technology Handbook (edited by the Laser Association, published by Asakura Shoten in 1984). FIG. 3 is a characteristic diagram showing the relationship with radius. As shown in the figure,
If the mirrors have radii of curvature bl and b2 and the distance between them is d, and one of the mirrors is rotated by θ, then the line connecting the centers of curvature of the mirrors is rotated by an angle φ. When the angle is small, the following equation holds.

b1θ=(b++b2 d)φ X= [b+ (b2 d)/ (b+b2 d)] 
BY= [b+b2/ (b++b2 d)]θここで
、X、  Yは鏡上のモード中心のずれである。
b1θ=(b++b2 d)φ X= [b+ (b2 d)/ (b+b2 d)]
BY=[b+b2/(b++b2 d)]θ where X and Y are the deviations of the mode center on the mirror.

上式より、例えば平行平面形(b+、b2→oo)のと
き、X、  Y、  はわずかなθに対しても非常に大
きなズレを生じる。逆に言えば、光を有効に利用するに
はミラーの位置決め精度は極めて高いことが要求される
。従来のミラーにおいては曲率半径は一定で、機械的な
位置決めによって光軸の調整を行っていた。
From the above equation, for example, in the case of a parallel plane type (b+, b2→oo), X, Y, cause a very large deviation even for a slight θ. Conversely, in order to utilize light effectively, the positioning accuracy of the mirror is required to be extremely high. In conventional mirrors, the radius of curvature is constant, and the optical axis is adjusted by mechanical positioning.

[発明が解決しようとする課題] 上記説明で明らかなように、曲率半径が一定である従来
のミラーを用いて光学系を構成する場合、まず光来照射
の常温状態で、静的に光軸な極めて高精度に定めること
が必要となる0次いで、光を照射したことによる温度変
化に伴う動的な光軸のズレを調整するのには熟練した技
術者の高度な技巧が求められ、非常に困難であるという
問題点があった。
[Problems to be Solved by the Invention] As is clear from the above explanation, when constructing an optical system using a conventional mirror with a constant radius of curvature, first, the optical axis is statically adjusted at room temperature during light irradiation. Adjusting the dynamic optical axis deviation due to temperature changes caused by irradiation of light requires the high level of skill of a skilled technician, and is extremely difficult. The problem was that it was difficult to

本発明は、上記のような問題点を解消するためになされ
たもので、熟練した技術者を必要とすることなく、簡便
に光学系の調整を行うための電気人力を加えることによ
り曲率半径を変えることができるミラーを得ることを目
的としており、従来のミラーにおいて不可能であった、
リアルタイムでの曲率半径の動的制御により、各種光学
機器の用途を大幅に広げ得るミラーを得ようとするもの
である。
The present invention was made to solve the above-mentioned problems, and it is possible to adjust the radius of curvature by applying electric power to easily adjust the optical system without requiring a skilled engineer. The aim is to obtain a mirror that can be changed, which was not possible with conventional mirrors.
By dynamically controlling the radius of curvature in real time, we aim to create a mirror that can greatly expand the applications of various optical instruments.

さらに本発明の別の発明は反射膜を高い付着力で形成で
きるミラーの製造方法を提供することを目的としている
Furthermore, another object of the present invention is to provide a method for manufacturing a mirror in which a reflective film can be formed with high adhesion.

[課題を解決するための手段] 本発明のミラーは、一面に反射膜を有する第1電歪素子
、第1電歪素子と歪方向をずらせて第1電歪素子の他面
と接合する第2電歪素子、第1電歪素子に電界を印加し
て第1電歪素子を歪ませる第1電界印加手段、及び第2
電歪素子に電界を印加して第2電歪素子を歪ませる第2
電界印加手段を備えたものである。
[Means for Solving the Problems] The mirror of the present invention includes a first electrostrictive element having a reflective film on one surface, a first electrostrictive element whose strain direction is shifted from the first electrostrictive element, and a first electrostrictive element joined to the other surface of the first electrostrictive element. 2 electrostrictive elements, a first electric field applying means for applying an electric field to the first electrostrictive element to distort the first electrostrictive element, and a second electrostrictive element;
A second device that applies an electric field to the electrostrictive element to distort the second electrostrictive element.
It is equipped with an electric field applying means.

また、本発明の別の発明のミラーの製造方法は第1電歪
素子の一面にイオンビーム蒸着法により反射膜を形成す
るようにしたものである。
Further, in another method of manufacturing a mirror according to the present invention, a reflective film is formed on one surface of the first electrostrictive element by ion beam evaporation.

[作用] 本発明のミラーは、電界を印加することによって歪ませ
る、膨張・収縮させることができる電歪素子を貼合わせ
た構造としているので、電気制御によるバイメタル効果
を実現することが可能となり、極めて高精度にミラー面
(反射膜)に凹凸を持たせることができる。即ち曲率半
径を変えることができる。
[Function] The mirror of the present invention has a structure in which electrostrictive elements that can be distorted, expanded and contracted by applying an electric field are bonded together, so it is possible to realize a bimetallic effect by electrical control. It is possible to create irregularities on the mirror surface (reflection film) with extremely high precision. That is, the radius of curvature can be changed.

本発明の別の発明のミラーの製造方法においては、イオ
ンビーム蒸着法により反射膜(ミラー面)を形成するよ
うにしたので、反射膜は第1ta歪素子に高い付着力で
付着し、上述の凹凸変化に対しても膜が剥離するといっ
た恐れがなく高い信頼性をもつミラーが形成できる。
In the method for manufacturing a mirror according to another aspect of the present invention, the reflective film (mirror surface) is formed by the ion beam evaporation method, so that the reflective film adheres to the first ta strain element with high adhesion force, resulting in the above-mentioned A mirror with high reliability can be formed without fear of the film peeling off even when unevenness changes.

[実施例] 以下、この発明の実施例を図面に基づいて説明する。[Example] Embodiments of the present invention will be described below based on the drawings.

第1図はこの発明の一実施例のミラーの構成を示す構成
図である。図において、(1)は平板状の第1電歪素子
で、一面にミラー面となる反射膜(4)、この場合は膜
厚0.3μIのAu蒸着膜が形成されている。(2)は
平板状の第2電歪素子で、第1電歪素子(1)の他面に
その歪方向が第1電歪素子(1)の歪方向と直交するよ
うに接合されている。(3)は接合層、この場合はエポ
キシ系接着剤、(5)は第1電歪素子(1)に電界を印
加して第1電歪素子(1)を歪ませる第1電界印加手段
、(6)は第2電歪素子(2)に電界を印加して第2電
歪素子(2)を歪ませる第2電界印加手段である。
FIG. 1 is a configuration diagram showing the configuration of a mirror according to an embodiment of the present invention. In the figure, (1) is a flat plate-shaped first electrostrictive element, on one surface of which a reflective film (4) serving as a mirror surface is formed, in this case an Au vapor-deposited film with a film thickness of 0.3 μI. (2) is a flat second electrostrictive element, which is bonded to the other surface of the first electrostrictive element (1) so that its strain direction is orthogonal to the strain direction of the first electrostrictive element (1). . (3) is a bonding layer, in this case an epoxy adhesive; (5) is a first electric field applying means for applying an electric field to the first electrostrictive element (1) to distort the first electrostrictive element (1); (6) is a second electric field applying means that applies an electric field to the second electrostrictive element (2) to distort the second electrostrictive element (2).

このように構成されたミラーにおいてミラー面に当たっ
た光の軸が可変できる原理を説明する。
The principle by which the axis of light hitting the mirror surface of a mirror configured in this way can be varied will be explained.

光軸可変制御、即ちミラーの形状を凹凸に制御するのは
、原理的にはバイメタル効果を応用することになるが、
以下にその一例について第1図および第2図をもとに説
明する。なお、第2図は第1図に示す実施例の動作を理
解しやすくするためのミラーの動作説明図である。周知
のように、電歪素子は電界を印加することによって、そ
の寸法を変化させる(歪む、膨張、収縮する)特性をも
っており、例えば無機系材料ではP Z T (Pt+
−Ti−Zr−0化合物)、また有機系ではポリフッ化
ビニリデン等の材料がすでに実用に供されている。この
場合はPZTを用いた。電界を印加していないスタート
時に、第2図の(A)または(A′)に示すごとく平板
状であった第1、第2電歪素子(1)(2)に、それぞ
れ第1電界印加手段(5)、第2電界印加手段(6)に
より 電界を印加することによって第2図の(B)また
は(8°)に示すように変形させることができる。これ
らの変形を総合することにより (C)のようにミラー
面を凹に変形させることが可能になる。なお、ミラー面
を凸に変形させるには、電界の印加方向を逆にすればよ
いことは明らかであり、第1電界印加手段(5)、第2
電界印加手段(6)より出力する電界を制御することに
より、その凹凸の度合、変形度を調節して、ミラー面を
所望の曲率に調整できる。従ってミラーの光軸を高精度
に定めるのに熟練した技術者を必要とせず、簡便にリア
ルタイムで位置決めでき、曲率半径の動的制御により、
各種光学機器の用途を大幅に広げ得る。
Variable optical axis control, that is, controlling the shape of the mirror to make it concave and convex, is based on the principle of applying the bimetal effect.
An example of this will be explained below based on FIGS. 1 and 2. Incidentally, FIG. 2 is an explanatory diagram of the operation of the mirror to facilitate understanding of the operation of the embodiment shown in FIG. 1. As is well known, an electrostrictive element has the property of changing its dimensions (distorting, expanding, contracting) by applying an electric field. For example, inorganic materials include P Z T (Pt+
-Ti-Zr-0 compounds), and organic materials such as polyvinylidene fluoride have already been put into practical use. In this case, PZT was used. At the start when no electric field is applied, a first electric field is applied to the first and second electrostrictive elements (1) and (2), which are flat as shown in (A) or (A') in Fig. 2, respectively. By applying an electric field using the means (5) and the second electric field applying means (6), it can be deformed as shown in (B) or (8°) in FIG. By combining these deformations, it becomes possible to deform the mirror surface into a concave shape as shown in (C). Note that in order to deform the mirror surface into a convex shape, it is clear that the direction of application of the electric field can be reversed.
By controlling the electric field output from the electric field applying means (6), the degree of unevenness and degree of deformation can be adjusted to adjust the mirror surface to a desired curvature. Therefore, there is no need for skilled technicians to determine the optical axis of the mirror with high precision, and positioning can be performed easily in real time, and by dynamic control of the radius of curvature,
The applications of various optical instruments can be greatly expanded.

なお、反射膜(4)の膜厚としては、500Å以上で反
射特性がでるので、5000Å以上になると第1電歪素
子(1)の繰り返し歪みにより クラックを生じたりす
る恐れがあるので、500〜5000人が適当である。
Note that the thickness of the reflective film (4) should be 500 Å or more since reflective properties are obtained, and if it is 5000 Å or more, cracks may occur due to repeated strain in the first electrostrictive element (1). 5,000 people is appropriate.

次に、別の発明のミラー製造方法の一実施例について説
明する。主にイオンビーム蒸着法による反射膜(ミラー
面)形成方法について説明する。
Next, an embodiment of a mirror manufacturing method according to another invention will be described. A method for forming a reflective film (mirror surface) mainly by ion beam evaporation will be described.

第3図はこの一実施例に係わるクラスタイオンビーム蒸
着装置の一例を示す構成図である。図において、(20
)は被蒸着材の第1電歪素子(1)と第2電歪素子(2
)が接合されたミラー基板、(4)は反射膜(蒸着膜)
、(8)は加速電極、(9)は蒸着材料、(10)はる
つぼ、(lりはるつぼ加熱ヒータ、(12)はイオン化
電極、(13)は真空槽である。
FIG. 3 is a configuration diagram showing an example of a cluster ion beam evaporation apparatus according to this embodiment. In the figure, (20
) are the first electrostrictive element (1) and the second electrostrictive element (2) of the material to be deposited.
) is bonded to the mirror substrate, (4) is the reflective film (deposited film)
, (8) is an accelerating electrode, (9) is a vapor deposition material, (10) is a crucible, (12) is an ionization electrode, (13) is a vacuum chamber.

まず、第1電歪素子(1)と第2電歪素子(2)をその
歪方向が互いに直交するように、エポキシ系接着剤で接
合したミラー基板を形成する。次にミラー基板の第1電
歪素子(1)の面に反射膜、この場合はAu膜をイオン
ビーム蒸着で形成する。最初に、真空[(13)をI 
0−6Torr程度に排気した後、るつぼ(10)をる
つぼ加熱ヒータ(11)により加熱し、るつぼ(10)
内の材料Auの蒸気圧がI Torr程度となるように
約1700℃(なお、例えばA1の場合は1600℃程
度)に加熱する。この状態で、るつぼ(10)からAu
蒸気のクラスタが噴出する。このクラスタにイオン化電
極(12)より電子シャワーを浴びせると、クラスタは
一部がイオン化される。クラスタイオンとなったAu蒸
気(7)は加速電極(8)によって運動エネルギを与え
られ、ミラー基板(20)上に衝突し、イオン化されな
かった中性のクラスタとともに膜形成にあずかる。この
際、膜形成の初期(膜厚50人程度まで)には少なくと
も加速電圧を3にV以上にして蒸着すると、クラスタイ
オンは大きな運動エネルギを与えられてミラー基板(2
0)に衝突し、ミラー基板(20)の表層とのミキシン
グ(表層イオン注入)層を形成する。このためミラー基
板(20)との付着力が強く、ミラーの曲率変化に対し
ても剥離等の恐れのない良好なミラー面を形成すること
ができる。また、加速電圧を3にV以上とすることで、
例えばAu反射膜(膜厚0.3μm)の場合、第4図の
反射率の加速電圧依存性を調べた実験結果を示す特性図
かられかるように、CO2レーザ光(波長10.6μm
)に対して、99.3%の極めて高い反射率を有するこ
とが実験の結果確かめられている。図の縦軸は反射率(
%)、横軸は加速電圧(Kv)である。
First, a mirror substrate is formed by bonding a first electrostrictive element (1) and a second electrostrictive element (2) with an epoxy adhesive such that their strain directions are perpendicular to each other. Next, a reflective film, in this case an Au film, is formed on the surface of the first electrostrictive element (1) of the mirror substrate by ion beam evaporation. First, the vacuum [(13) is
After exhausting the air to about 0-6 Torr, the crucible (10) is heated by the crucible heating heater (11), and the crucible (10)
It is heated to about 1700° C. (for example, about 1600° C. in the case of A1) so that the vapor pressure of the material Au inside becomes about I Torr. In this state, Au is removed from the crucible (10).
Clusters of steam erupt. When this cluster is showered with electrons from an ionizing electrode (12), a portion of the cluster is ionized. The Au vapor (7), which has become cluster ions, is given kinetic energy by the accelerating electrode (8), collides with the mirror substrate (20), and participates in film formation together with neutral clusters that have not been ionized. At this time, if the accelerating voltage is set to at least 3 V or higher during the initial stage of film formation (up to a film thickness of about 50), the cluster ions will be given a large kinetic energy and the mirror substrate (2
0) to form a mixing (surface layer ion implantation) layer with the surface layer of the mirror substrate (20). Therefore, the adhesion to the mirror substrate (20) is strong, and a good mirror surface can be formed without fear of peeling even when the curvature of the mirror changes. In addition, by setting the acceleration voltage to 3 V or higher,
For example, in the case of an Au reflective film (film thickness 0.3 μm), as can be seen from the characteristic diagram showing the experimental results of investigating the dependence of reflectance on accelerating voltage in Figure 4, CO2 laser light (wavelength 10.6 μm)
), it has been confirmed through experiments that it has an extremely high reflectance of 99.3%. The vertical axis of the figure is the reflectance (
%), and the horizontal axis is the acceleration voltage (Kv).

ちなみに、真空蒸着法では99.0%以下(通常98.
8%)の低い反射率である。加速電圧は、膜の付着力、
反射率の点から3にV以上が、また7にV以上になると
基板が荒れる、膜の付着効率が低下するなどの点から3
〜7Kvが望ましい。この場合は、膜厚50人までは加
速電圧5Kvで、それ以後は3Kvで、0.3μmのA
u反射膜を形成した。  なお、付着力をさらに高める
目的で、蒸着前にAr”やNo等の不活性なガスイオン
の照射を行い、基板表面の吸着物を取り除き、活性化さ
れた清浄なミラー基板面を作り、この上に膜形成するの
も有効である。
By the way, in the vacuum evaporation method, it is 99.0% or less (usually 98.
8%). The acceleration voltage is the adhesion force of the film,
3 from the viewpoint of reflectance, and 3 from the point of view that if it exceeds V, the substrate will become rough and the film adhesion efficiency will decrease.
~7Kv is desirable. In this case, the acceleration voltage is 5Kv until the film thickness reaches 50 people, and after that, the acceleration voltage is 3Kv, and the A of 0.3μm is applied.
A u reflective film was formed. In addition, in order to further increase the adhesion force, irradiation with inert gas ions such as Ar and No is performed before vapor deposition to remove adsorbed matter on the substrate surface and create an activated and clean mirror substrate surface. It is also effective to form a film thereon.

なお、上記実施例では、平面鏡の場合について説明した
が、凹面鏡、凸面鏡でも同様の効果を奏することは明か
である。
Although the above embodiments have been explained using a plane mirror, it is clear that the same effect can be achieved using a concave mirror or a convex mirror.

[発明の効果] 以上のように、本発明によれば、一面に反射膜を有する
第1電歪素子、第1電歪業子と歪方向をずらせて第1電
歪素子の他面と接合する第2電歪素子、第1電歪素子に
電界を印加して第1電歪素子を歪ませる第1電界印加手
段、及び第2電歪素子に電界を印加して第2電歪素子を
歪ませる第2電界印加手段を備えたミラーにすることに
より、リアルタイムで簡便にミラーの曲率を変えること
ができる効果がある。
[Effects of the Invention] As described above, according to the present invention, the first electrostrictive element has a reflective film on one surface, and the first electrostrictive element is bonded to the other surface of the first electrostrictive element with the strain direction shifted. a second electrostrictive element that applies an electric field to the first electrostrictive element to distort the first electrostrictive element; and a first electric field applying means that applies an electric field to the second electrostrictive element to distort the first electrostrictive element; By using a mirror equipped with a means for applying a second electric field for distortion, there is an effect that the curvature of the mirror can be easily changed in real time.

また、本発明の別の発明によれば、第1電歪素子の一面
にイオンビーム蒸着法により反射膜を形成することによ
り、ミラーの曲率の変化に対応できる十分に強い付着力
をもったミラーを形成でき、長期信頼性に優れた光軸可
変ミラーが得られる効果がある。
According to another aspect of the present invention, by forming a reflective film on one surface of the first electrostrictive element by ion beam evaporation, the mirror has a sufficiently strong adhesion force that can cope with changes in the curvature of the mirror. This has the effect of providing a variable optical axis mirror with excellent long-term reliability.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの発明の一実施例のミラーを示す構成図、第
2図は第1図のミラーの動作説明図、第3図はこの発明
に係わるクラスタイオンビーム蒸着装置を示す構成図、
第4図はこの発明に係わる反射率の加速電圧依存性を示
す特性図、第5図は従来の光学素子における光軸と曲率
半径との関係を示す説明図である。 区において、(1)は第1電歪素子、(2)は第2電歪
素子、(3)は接合層、(4)は反射膜、(5)は第1
電界印加手段、(6)は第2電界印加手段である。 なお、各図中、同一符号は同一または相当部分を示す。
FIG. 1 is a block diagram showing a mirror according to an embodiment of the present invention, FIG. 2 is an explanatory diagram of the operation of the mirror in FIG. 1, and FIG. 3 is a block diagram showing a cluster ion beam evaporation apparatus according to the present invention.
FIG. 4 is a characteristic diagram showing the dependence of reflectance on accelerating voltage according to the present invention, and FIG. 5 is an explanatory diagram showing the relationship between the optical axis and the radius of curvature in a conventional optical element. (1) is the first electrostrictive element, (2) is the second electrostrictive element, (3) is the bonding layer, (4) is the reflective film, and (5) is the first electrostrictive element.
The electric field applying means (6) is a second electric field applying means. In each figure, the same reference numerals indicate the same or corresponding parts.

Claims (2)

【特許請求の範囲】[Claims] (1)一面に反射膜を有する第1電歪素子、第1電歪素
子と歪方向をずらせて第1電歪素子の他面と接合する第
2電歪素子、第1電歪素子に電界を印加して第1電歪素
子を歪ませる第1電界印加手段、及び第2電歪素子に電
界を印加して第2電歪素子を歪ませる第2電界印加手段
を備えたミラー。
(1) A first electrostrictive element having a reflective film on one surface, a second electrostrictive element joined to the other surface of the first electrostrictive element with the strain direction shifted from the first electrostrictive element, and an electric field applied to the first electrostrictive element. A mirror comprising a first electric field applying means for applying an electric field to distort the first electrostrictive element, and a second electric field applying means for applying an electric field to the second electrostrictive element to distort the second electrostrictive element.
(2)第1電歪素子の一面にイオンビーム蒸着法により
反射膜を形成するようにした請求項1記載のミラーの製
造方法。
(2) The method for manufacturing a mirror according to claim 1, wherein a reflective film is formed on one surface of the first electrostrictive element by ion beam evaporation.
JP14289488A 1988-06-10 1988-06-10 Mirror and production thereof Pending JPH01312505A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14289488A JPH01312505A (en) 1988-06-10 1988-06-10 Mirror and production thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14289488A JPH01312505A (en) 1988-06-10 1988-06-10 Mirror and production thereof

Publications (1)

Publication Number Publication Date
JPH01312505A true JPH01312505A (en) 1989-12-18

Family

ID=15326073

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14289488A Pending JPH01312505A (en) 1988-06-10 1988-06-10 Mirror and production thereof

Country Status (1)

Country Link
JP (1) JPH01312505A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010210681A (en) * 2009-03-06 2010-09-24 Mitsubishi Electric Corp Mirror and production method of the same
US7832879B2 (en) 2004-09-21 2010-11-16 Bae Systems Plc Heat dissipating layers in deformable mirrors
JP2016057529A (en) * 2014-09-11 2016-04-21 株式会社デンソー 3D shape creation device
JP2017114393A (en) * 2015-12-25 2017-06-29 株式会社デンソー Drive support display device and display system

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7832879B2 (en) 2004-09-21 2010-11-16 Bae Systems Plc Heat dissipating layers in deformable mirrors
JP2010210681A (en) * 2009-03-06 2010-09-24 Mitsubishi Electric Corp Mirror and production method of the same
JP2016057529A (en) * 2014-09-11 2016-04-21 株式会社デンソー 3D shape creation device
JP2017114393A (en) * 2015-12-25 2017-06-29 株式会社デンソー Drive support display device and display system

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