JPH0445811B2 - - Google Patents
Info
- Publication number
- JPH0445811B2 JPH0445811B2 JP57019222A JP1922282A JPH0445811B2 JP H0445811 B2 JPH0445811 B2 JP H0445811B2 JP 57019222 A JP57019222 A JP 57019222A JP 1922282 A JP1922282 A JP 1922282A JP H0445811 B2 JPH0445811 B2 JP H0445811B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- polarizing
- electro
- beam splitter
- plzt
- 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.)
- Expired - Lifetime
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/03—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect
- G02F1/055—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect the active material being a ceramic
Landscapes
- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Ceramic Engineering (AREA)
- Nonlinear Science (AREA)
- Crystallography & Structural Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Dot-Matrix Printers And Others (AREA)
- Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)
- Laser Beam Printer (AREA)
- Exposure Or Original Feeding In Electrophotography (AREA)
Description
【発明の詳細な説明】
本発明は光シヤツタとして用いられる電気光学
素子に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electro-optical element used as an optical shutter.
従来、電気光学素子は特開昭55−147611号公報
などに示されているように強誘電体にPLZTを用
い、これをはさむ様に配置される2個の偏光素子
に偏光板を用いている。この偏光板は通常高分子
フイルムで構成され、この偏光フイルムはポリビ
ニルアルコールを引き伸ばし分子をその伸ばした
方向に並ばせた後ヨウ素を含んだ溶液に浸しヨウ
素をしみ込ませて長い鎮をつくり洗つて乾燥する
ことにより得られ、ポラロイド社のHN38などが
ポピユラーなものである。しかしこの電気光学素
子では偏光フイルム例えばポラロイド社のHN38
は入射光に対して直線偏光成分としてとり出せる
成分が約38%であり、PLZTの後側に配置された
もので偏光方向がPLZTからの入射光の振動方向
に一致した場合でも約76%の光しか通過せぐ、
PLZTの前後に配置された2枚の偏光フイルムを
透過する光は約29%になり光の利用効率が非常に
悪い。 Conventionally, electro-optical elements use PLZT as a ferroelectric material, and a polarizing plate is used as two polarizing elements arranged to sandwich the ferroelectric material, as shown in Japanese Unexamined Patent Publication No. 147611/1983. . This polarizing plate is usually composed of a polymer film, and this polarizing film is made by stretching polyvinyl alcohol so that the molecules are aligned in the stretched direction, then soaking it in an iodine-containing solution to make a long film, washing it, and drying it. Popular products include Polaroid's HN38. However, with this electro-optical element, polarizing film such as Polaroid's HN38
About 38% of the incident light can be extracted as a linearly polarized component, and even if it is placed behind the PLZT and the polarization direction matches the vibration direction of the incident light from the PLZT, about 76% of the component can be extracted as a linearly polarized component. Only light can pass through,
Approximately 29% of the light passes through the two polarizing films placed before and after the PLZT, which is extremely inefficient.
本発明は上記のような欠点を改善し、2個の偏
光素子の少くとも一方を偏光ビームスプリツタで
構成することにより光の利用効率向上を計つた電
気光学素子を提供することを目的とする。 SUMMARY OF THE INVENTION An object of the present invention is to improve the above-mentioned drawbacks and provide an electro-optical element that improves light utilization efficiency by configuring at least one of two polarizing elements as a polarizing beam splitter. .
以下図面を参照しながら本発明について実施例
をあげて説明する。 The present invention will be described below by way of examples with reference to the drawings.
第1図は電気光学素子の一例を示す。この電気
光学素子は光シヤツタを構成するもので、PLZT
等の透光性セラミツクス1と偏光素子2,3とよ
りなる。透明な強誘電性セラミツクのPLZT
〔(Pb,La)(Zr,Ti)O3磁器の略称〕はその組
成が(Pb1−xLAx)(Zr1−yTiy)O3の化学式で
示される。このPLZTはその組成により1次、2
次の電気光学効果および光学的メモリ効果をもつ
ことから光シヤツタ、デイスプレイ等の電気光学
分野への応用が研究されている。なかでもPLZT
(x/65/35,x=8.6〜10.0)は常温では常誘電
性を示すが、直流電圧を加えると強誘電相が誘起
され2次電気光学効果いわゆるKerr効果を示す
ようになる。この種のものは記憶機能がないの
で、光シヤツタへの応用をに適しており、スリム
ループ2次電気光学材料と呼ばれている。透光性
セラミツク1は例えばそのスリムループ2次電気
光学材料のPLZTが用いられ、偏光素子2,3は
PLZT1の前後にこれをはさむ様に配置される。
偏光素子2,3の偏光方向は直交し、PLZT1は
電圧印加方向が入射する直線偏光の振動面に対し
て45°の傾きをもつている。PLZT1の電極4,
5間に電圧が印加されない時には光源の照明光は
偏光素子2により直線偏光成分がとり出されて
PLZT1を通過するが、偏光素子3により遮断さ
れる。電極4,5間に電圧が加えられると、偏光
素子2からの直線偏光はPLZT1における電極
4,5間の光シヤツタ部でKerr効果により振動
方向が90°回転されて偏光素子3を通過し、その
通過光量Iは
I=Ipsin2(t△n/λ)r
で表わされる。ここではIpはPLZT1の入射直線
偏光の光量、tはPLZT1の厚さ、λはPLZT1
の透過光の波長、△nはPLZT1の屈折率の光軸
方向成分neとこれに垂直な常光に対する屈折率np
との差)np−ne)である。Iが最大になる電圧を
半波長電圧という。従つてこの光シヤツタは電極
4,5間に電圧を加えない時にオフとなり、電極
4,5間に電圧を加えた時にオンとなる。 FIG. 1 shows an example of an electro-optical element. This electro-optical element constitutes an optical shutter, and PLZT
It consists of a translucent ceramic 1 and polarizing elements 2 and 3. PLZT transparent ferroelectric ceramic
The composition of [(Pb, La) (Zr, Ti) O 3 porcelain abbreviation] is shown by the chemical formula (Pb 1 −xLAx)(Zr 1 −yTiy)O 3 . This PLZT is primary or secondary depending on its composition.
Since it has the following electro-optic effect and optical memory effect, its application to electro-optic fields such as optical shutters and displays is being studied. Especially PLZT
(x/65/35, x = 8.6 to 10.0) exhibits paraelectricity at room temperature, but when a DC voltage is applied, a ferroelectric phase is induced and a secondary electro-optic effect, the so-called Kerr effect, is exhibited. Since this type of material does not have a memory function, it is suitable for application in optical shutters and is called a slim-loop secondary electro-optic material. For example, PLZT, a slim loop secondary electro-optic material, is used as the translucent ceramic 1, and the polarizing elements 2 and 3 are
This is placed before and after PLZT1.
The polarization directions of the polarizing elements 2 and 3 are perpendicular to each other, and the voltage application direction of the PLZT 1 is inclined at 45° with respect to the vibration plane of the incident linearly polarized light. Electrode 4 of PLZT1,
When no voltage is applied between 5, the linearly polarized component of the illumination light from the light source is extracted by the polarizing element
It passes through the PLZT 1 but is blocked by the polarizing element 3. When a voltage is applied between the electrodes 4 and 5, the linearly polarized light from the polarizing element 2 is rotated by 90 degrees in the vibration direction due to the Kerr effect at the optical shutter section between the electrodes 4 and 5 in the PLZT 1, and passes through the polarizing element 3. The amount of passing light I is expressed as I=I p sin 2 (tΔn/λ)r. Here, I p is the amount of linearly polarized light incident on PLZT1, t is the thickness of PLZT1, and λ is PLZT1
The wavelength of the transmitted light, △n is the optical axis direction component of the refractive index of PLZT1 n e and the refractive index for ordinary light perpendicular to this n p
n p − n e ). The voltage at which I is maximum is called the half-wavelength voltage. Therefore, this light shutter is turned off when no voltage is applied between the electrodes 4 and 5, and turned on when a voltage is applied between the electrodes 4 and 5.
第2図は光シヤツタアレイを構成する電気光学
素子の従来例を示す。この例ではPLZT1上に複
数の信号電極41〜44と共通電極5が設けられて
おり、信号電極41〜44のうちの電圧が印加され
たものと共通電極5との間の光シヤツタ部のみが
Kerr効果を示してオンする。 FIG. 2 shows a conventional example of an electro-optical element constituting an optical shutter array. In this example, a plurality of signal electrodes 4 1 to 4 4 and a common electrode 5 are provided on the PLZT 1, and light between the signal electrodes 4 1 to 4 4 to which voltage is applied and the common electrode 5 is provided. Only the shutter part
Show Kerr effect and turn on.
この従来例では、PLZT1における光シヤツタ
部は複数の信号電極41,42…と共通電極5との
間に複数個形成され、横方向へ一列に配列され
る。このため、例えば斜線はPLZT1の各光シヤ
ツタ部を通過した光により第14図に示すように
複数の画素111,112…,121,122…で構成さ
れて端縁がギザギザになり斜線の再現性が悪くな
る。 In this conventional example, a plurality of optical shutter portions in the PLZT 1 are formed between the plurality of signal electrodes 4 1 , 4 2 . . . and the common electrode 5, and are arranged in a row in the horizontal direction. For this reason, for example, the diagonal line is composed of a plurality of pixels 1 11 , 1 12 . The reproducibility of diagonal lines deteriorates.
第3図は本発明の第1の実施例を示す。この実
施例では第2図の従来例において後側の偏光素子
が偏光ビームスプリツタ6で構成され、PLZT1
上には2組の電極41,42…51,52…が偏光素
子2,6を通過する光の振動方向に対して約45°
の傾きを持つ様に設けられている。PLZT1及び
偏光素子2,6よりなる電気光学素子は光源7に
より照明される。第4図に示すように光源7から
の光は偏光板2で紙面に垂直な方向の振動成分の
みがとり出され、PLZT1における2組の電極4
1,42…,51,52…の間、の電界が印加された
光シヤツタ部でKerr効果により振動方向が90°回
転して偏光ビームスプリツタ6を透過する。
PLZT1の電界が印加されていない部分を通過し
た直線偏光はビームスプリツタ6で約90°偏光
される。なお、第4図以下で黒丸印は光の振動方
向が紙面に垂直であることを示し、正逆方向を示
す矢印は光の振動方向が紙面に平行であることを
示す。 FIG. 3 shows a first embodiment of the invention. In this embodiment, unlike the conventional example shown in FIG. 2, the rear polarizing element is composed of a polarizing beam splitter 6,
Above, two sets of electrodes 4 1 , 4 2 . . . 5 1 , 5 2 .
It is set up so that it has an inclination of . The electro-optical element consisting of the PLZT 1 and the polarizing elements 2 and 6 is illuminated by a light source 7. As shown in FIG. 4, only the vibration component of the light from the light source 7 in the direction perpendicular to the paper is extracted by the polarizing plate 2, and the two sets of electrodes 4 in the PLZT 1
1 , 4 2 . . . , 5 1 , 5 2 . . . , the vibration direction is rotated by 90° due to the Kerr effect at the optical shutter portion to which the electric field is applied, and the beam is transmitted through the polarizing beam splitter 6 .
The linearly polarized light that has passed through the part of the PLZT 1 to which no electric field is applied is polarized by about 90 degrees by the beam splitter 6. Note that in FIG. 4 and subsequent figures, black circles indicate that the direction of vibration of light is perpendicular to the plane of paper, and arrows indicating forward and reverse directions indicate that the direction of vibration of light is parallel to the plane of paper.
この実施例では、2組の電極41,42…,51,
52…はPLZT1の一方の面に配置し、かつ、
PLZT1を通過する光の振動方向に対して約45度
の傾きを持つように配置されている。このため、
PLZT1における2組の電極41,42…,51,5
2…の各間に形成される光シヤツタ部は約45度の
傾きを持つ斜め向きの複数個の光シヤツタ部で構
成され、例えば斜線はPLZT1の斜め向きの光シ
ヤツタ部を通過した光により第13図に示すよう
に斜め向きの画素111,112…,121,122…で
構成されて端縁がギザギザにならずに斜線の再現
性が良くなる。 In this embodiment, two sets of electrodes 4 1 , 4 2 . . . , 5 1 ,
5 2 ... is placed on one side of PLZT1, and
It is arranged to have an inclination of approximately 45 degrees with respect to the vibration direction of light passing through PLZT1. For this reason,
Two sets of electrodes 4 1 , 4 2 ..., 5 1 , 5 in PLZT1
2. The light shutter section formed between each of is composed of a plurality of oblique light shutter sections having an inclination of approximately 45 degrees. For example, the diagonal lines indicate that the light passing through the oblique light shutter section of PLZT1 As shown in FIG. 13, it is composed of diagonally oriented pixels 1 11 , 1 12 . . . , 1 21 , 1 22 .
第5図は本発明の第2の実施例を示す。この実
施例は第1の実施例において偏光板2と偏光板ビ
ームスプリツタ6の配置を逆にしたものである。 FIG. 5 shows a second embodiment of the invention. In this embodiment, the arrangement of the polarizing plate 2 and the polarizing plate beam splitter 6 is reversed in the first embodiment.
第6図は本発明の第3の実施例を示す。この実
施例は上記実施例において2個の偏光素子とも偏
光ビームスプリータ6,8で構成したものであ
り、光源7と光軸と電気光学素子の光を出射する
光軸とが約90°の角度をもつ。 FIG. 6 shows a third embodiment of the invention. In this embodiment, both of the two polarizing elements in the above embodiment are composed of polarizing beam splitters 6 and 8, and the light source 7, the optical axis, and the optical axis from which the light of the electro-optic element is emitted are approximately 90 degrees apart. Has an angle.
第7図は本発明の第4の実施例を示す。この実
施例は第3の実施例において光源7の光軸を
PLZT1の光軸と約90°の角度をもたせたもので
ある。 FIG. 7 shows a fourth embodiment of the invention. This embodiment differs from the third embodiment in that the optical axis of the light source 7 is
It has an angle of approximately 90° with the optical axis of PLZT1.
第8図は上記の如き本発明による電気光学素子
10を用いた記録装置の一例を示す。感光体ドラ
ム11は駆動装置により回転駆動され、帯電部1
2により一様に帯電された後に電気光学素子10
により光像が照射されて潜像が形成される。電気
光学素子10は光シヤツタアレイを構成するもの
で、感光体ドラム11の幅方向に配置され、2組
の電極41,42…,51,52…の対応するもの同
志の間に各々の画素信号が加えられて光源7から
の光を変調する。電気光学素子10から出射され
る光像は出射後に拡がつてしまうため、電気光学
素子10と感光体ドラム11とのギヤツプは100
〜200μ程度に保持する必要がある。感光体ドラ
ム11上の潜像は現像部13で現像され、給紙装
置からの転写紙へ転写部14により転写される。
この転写紙は定着部で画像が定着され、また感光
体ドラム11は画像転写後に除電部15で除電さ
れてクリーニング部16で清掃される。第9図に
示すように電気光学素子10の出射光像は集束性
光伝送体、ダハミラーレンズアレイなどの等倍結
像素子17で感光体ドラム11上に結像してもよ
い。 FIG. 8 shows an example of a recording apparatus using the electro-optical element 10 according to the present invention as described above. The photosensitive drum 11 is rotationally driven by a driving device, and the charging section 1
After being uniformly charged by 2, the electro-optical element 10
A latent image is formed by irradiating a light image. The electro-optical element 10 constitutes an optical shutter array, is arranged in the width direction of the photoreceptor drum 11, and is arranged between corresponding electrodes of two sets of electrodes 4 1 , 4 2 . . . , 5 1 , 5 2 . is applied to modulate the light from the light source 7. Since the optical image emitted from the electro-optical element 10 spreads after being emitted, the gap between the electro-optical element 10 and the photoreceptor drum 11 is 100.
It is necessary to keep it at around ~200μ. The latent image on the photosensitive drum 11 is developed by a developing section 13, and transferred by a transfer section 14 onto a transfer sheet from a paper feeding device.
The image is fixed on the transfer paper by a fixing section, and after the image is transferred, the photosensitive drum 11 is neutralized by a charge eliminating section 15 and cleaned by a cleaning section 16. As shown in FIG. 9, the light image emitted from the electro-optical element 10 may be formed on the photoreceptor drum 11 by a 1-magnification imaging element 17 such as a focusing light transmitter or a roof mirror lens array.
第10図は上記実施例で用いた偏光ビームスプ
リツタの構造を示す。この偏光ビームスプリツタ
はガラスなど透明材料よりなる直角プリズム1
8,19の一方または両方にガラス材料よりも屈
折率の高い物質20と屈折率の低い物質21とを
交互に蒸着法などにより形成し、これらを接着剤
22ではり合わせたものである。 FIG. 10 shows the structure of the polarizing beam splitter used in the above embodiment. This polarizing beam splitter consists of a right-angle prism 1 made of a transparent material such as glass.
A substance 20 having a higher refractive index than a glass material and a substance 21 having a lower refractive index are alternately formed on one or both of the glass materials by vapor deposition or the like, and these are glued together with an adhesive 22.
第11図はこの偏光ビームスプリツタの作用を
示す。入射光は偏光ビームスプリツタの入射面に
平行なP成分が偏光ビームスプリツタをほぼ100
%近く通過し、偏光ビームスプリツタの入射面に
垂直なS成分が偏光ビームスプリツタでほぼ100
%近く反射される。 FIG. 11 shows the operation of this polarizing beam splitter. The incident light has a P component parallel to the plane of incidence of the polarizing beam splitter, which is approximately 100
%, and the S component perpendicular to the plane of incidence of the polarizing beam splitter is approximately 100%.
% is reflected.
第12図は偏光ビームスプリツタ及び光源7の
波長分布の例を示す。偏光ビームスプリツタはガ
ラス材料の屈折率が1.52、物質20の屈折率が
1.58、物質21の屈折率が1.46で物質20,21
が約195μmの光学的膜厚に交互に49層に形成さ
れている。この偏光ビームスプリツタは約550n
mを中心に±30nmの幅で入射光のP成分とS成
分を分離する。この分離可能な範囲内でグリーン
発光するけい光灯(アパーチヤ型が望ましい)を
光源7として用いれば光を非常に有効に利用でき
る。 FIG. 12 shows an example of the wavelength distribution of the polarizing beam splitter and the light source 7. In the polarizing beam splitter, the refractive index of the glass material is 1.52, and the refractive index of the material 20 is
1.58, the refractive index of substance 21 is 1.46, and substances 20 and 21
are alternately formed in 49 layers with an optical thickness of approximately 195 μm. This polarizing beam splitter is about 550n
Separate the P component and S component of the incident light with a width of ±30 nm centered on m. If a fluorescent lamp (preferably an aperture type) that emits green light within this separable range is used as the light source 7, the light can be used very effectively.
光の利用効率について例示すると、偏光フイル
ムを2枚用いた従来例では光は光源の出射光
(100%)→偏光フイルムの透過光(38%)→
PLZTの透過光(25%)→偏光フイルムの透過光
(19%)となる。これに対し偏光ビームスプリツ
タを2個用いた上記実施例では光源の出射光
(100%)→偏光ビームスプリツタの透過光(50
%)→PLZTの透過光(33%)→偏光ビームスプ
リツタの透過光(33%)となり、光の利用効率は
従来例に比べて約70%向上する。 To give an example of light utilization efficiency, in a conventional example using two polarizing films, the light is emitted from the light source (100%) → transmitted light through the polarizing film (38%) →
Light transmitted through PLZT (25%) → light transmitted through polarizing film (19%). On the other hand, in the above embodiment using two polarizing beam splitters, the light emitted from the light source (100%) → the transmitted light of the polarizing beam splitter (50%)
%) → light transmitted through the PLZT (33%) → light transmitted through the polarizing beam splitter (33%), improving light utilization efficiency by approximately 70% compared to the conventional example.
以上のように本発明によれば電気光学素子にお
いて2個の偏光素子の少くとも一方を偏光ビーム
スプリツタで構成したので、光の利用効率を向上
させることができ、また偏光ビームスプリツタで
光路の変換ができ光学的レイアウトを自由度が向
上する。しかも、強誘電体に設けられた複数個の
電極は、強誘電体の一方の面に配置されているの
で、光が強誘電体光における電極間の光シヤツタ
部を通過し、光が強誘電体を通過する際に電極の
通過による損失がない。さらに、強誘電体に設け
られた複数個の電極は、偏光素子を透過する光の
振動方向に対して約45度の傾きを持つように配置
されているので、斜線の再現性が良くなる。 As described above, according to the present invention, at least one of the two polarizing elements in the electro-optical element is configured with a polarizing beam splitter, so that the efficiency of light utilization can be improved, and the polarizing beam splitter can also be used to divide the optical path. The degree of freedom in optical layout is improved. Moreover, since the plurality of electrodes provided on the ferroelectric material are arranged on one surface of the ferroelectric material, the light passes through the light shutter section between the electrodes in the ferroelectric light, and the light passes through the ferroelectric light. There is no loss due to the passage of the electrode as it passes through the body. Furthermore, since the plurality of electrodes provided on the ferroelectric material are arranged so as to have an inclination of about 45 degrees with respect to the vibration direction of light transmitted through the polarizing element, the reproducibility of diagonal lines is improved.
第1図は光シヤツタの一例を示す斜視図、第2
図は従来の光シヤツタアレイを示す斜視図、第3
図及び第4図は本発明の一実施例を示す斜視図及
び正面図、第5図〜第7図は本発明の他の各実施
例を示す正面図、第8図は記録装置の一例を示す
概略図、第9図は記録装置の他の例の一部を示す
概略図、第10図は偏光ビームスプリツタを一例
の構成説明図、第11図は偏光ビームスプリツタ
の作用説明図、第12図は偏光ビームスプリツタ
と光源の波長分布の例を示す図、第13図は従来
例の斜線再現例を示す図、第14図は上記実施例
の斜線再現例を示す図である。
1……PLZT、2……偏光素子、6,8……偏
光ビームスプリツタ。
Figure 1 is a perspective view showing an example of a light shutter;
The figure is a perspective view showing a conventional optical shutter array.
4 are a perspective view and a front view showing one embodiment of the present invention, FIGS. 5 to 7 are front views showing other embodiments of the present invention, and FIG. 8 is an example of a recording device. FIG. 9 is a schematic diagram showing a part of another example of the recording device, FIG. 10 is a configuration explanatory diagram of an example of a polarizing beam splitter, and FIG. 11 is an explanatory diagram of the operation of the polarizing beam splitter. FIG. 12 is a diagram showing an example of wavelength distribution of a polarizing beam splitter and a light source, FIG. 13 is a diagram showing an example of reproducing diagonal lines in the conventional example, and FIG. 14 is a diagram showing an example of reproducing diagonal lines in the above embodiment. 1...PLZT, 2...Polarizing element, 6, 8...Polarizing beam splitter.
Claims (1)
誘電体をはさむ様に配置された2個の偏光素子と
を備え、この2個の偏光素子の少くとも一方を偏
光ビームスプリツタで構成し、前記強誘電体に設
けられた複数個の電極は、前記強誘電体の一方の
面に配置され、かつ、前記偏光素子を通過する光
の振動方向に対して約45度の傾きを持つように配
置されたことを特徴とする電気光学素子。1. Comprising a ferroelectric material exhibiting a secondary electro-optic effect and two polarizing elements arranged to sandwich this ferroelectric material, at least one of these two polarizing elements is configured with a polarizing beam splitter. The plurality of electrodes provided on the ferroelectric material are arranged on one surface of the ferroelectric material and have an inclination of about 45 degrees with respect to the vibration direction of the light passing through the polarizing element. An electro-optical element characterized in that it is arranged as follows.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57019222A JPS58136016A (en) | 1982-02-09 | 1982-02-09 | Electrooptic element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57019222A JPS58136016A (en) | 1982-02-09 | 1982-02-09 | Electrooptic element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58136016A JPS58136016A (en) | 1983-08-12 |
| JPH0445811B2 true JPH0445811B2 (en) | 1992-07-28 |
Family
ID=11993335
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57019222A Granted JPS58136016A (en) | 1982-02-09 | 1982-02-09 | Electrooptic element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58136016A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4765721A (en) * | 1987-09-23 | 1988-08-23 | Eastman Kodak Company | Stress-tolerant light valve array construction |
| US5054893A (en) * | 1990-08-17 | 1991-10-08 | Schoonscan, Inc. | Electro-optic cell linear array |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5723918A (en) * | 1980-07-18 | 1982-02-08 | Ricoh Co Ltd | Optical switch |
-
1982
- 1982-02-09 JP JP57019222A patent/JPS58136016A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58136016A (en) | 1983-08-12 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5239322A (en) | Display apparatus | |
| JP3514533B2 (en) | Image projection system | |
| US5093874A (en) | Integrated electro-optical scanner with photoconductive substrate | |
| JPS6026316A (en) | Image forming device | |
| JPH0445811B2 (en) | ||
| US4763996A (en) | Spatial light modulator | |
| US5159456A (en) | Photo-to-photo transducer and method of operation using a photo-moldulation member affected by a change distribution in a photoconductive member and a voltage applied across electrodes | |
| JP3733805B2 (en) | Image copying machine | |
| JPS58130321A (en) | Optical switching array element | |
| JP3783117B2 (en) | Image recording device | |
| JPS6375727A (en) | Optical shutter | |
| JPH0228620A (en) | Liquid crystal shutter | |
| JPS597337A (en) | optical control device | |
| JPS60200224A (en) | image exposure device | |
| JPS5917528A (en) | optical control device | |
| EP0657764B1 (en) | Photo-to-photo transducer | |
| JPS597338A (en) | Optical controller | |
| JPS5910927A (en) | Optical controller | |
| JPS5915918A (en) | optical control device | |
| JPH02115813A (en) | Optical system equipped with liquid crystal element | |
| JPH0463320A (en) | Photo-photo conversion element | |
| JPS63189265A (en) | Image recorder | |
| JPS58209720A (en) | Liquid crystal display device | |
| JPS61177427A (en) | Optical system using physical shutter | |
| JPS63253919A (en) | Optical image conversion device |