JPS59128518A - Liquid crystal light valve - Google Patents

Liquid crystal light valve

Info

Publication number
JPS59128518A
JPS59128518A JP58004587A JP458783A JPS59128518A JP S59128518 A JPS59128518 A JP S59128518A JP 58004587 A JP58004587 A JP 58004587A JP 458783 A JP458783 A JP 458783A JP S59128518 A JPS59128518 A JP S59128518A
Authority
JP
Japan
Prior art keywords
liquid crystal
light valve
crystal light
electrode
signal
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
JP58004587A
Other languages
Japanese (ja)
Inventor
Harukazu Matsushita
松下 晴計
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.)
Seiko Epson Corp
Suwa Seikosha KK
Original Assignee
Seiko Epson Corp
Suwa Seikosha KK
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 Seiko Epson Corp, Suwa Seikosha KK filed Critical Seiko Epson Corp
Priority to JP58004587A priority Critical patent/JPS59128518A/en
Publication of JPS59128518A publication Critical patent/JPS59128518A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/13Devices 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 liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/13306Circuit arrangements or driving methods for the control of single liquid crystal cells

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  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Liquid Crystal (AREA)
  • Mathematical Physics (AREA)
  • Chemical & Material Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)

Abstract

PURPOSE:To constitute a liquid crystal light valve that can furnish a light writing unit of high performance and low price by enabling the liquid crystal light valve 1/3 time division driving. CONSTITUTION:Selection signals 221-223 are applied to three common electrodes 201-203. Open or close signal 225, 226 is applied to a signal electrode 205 according to write data. At this time, signals 221-224 and signals 225-226 are reverse in phase. Microshutters 211-213 are opened and closed according to signals applied to the signal electrode during the time of selection of signals 221-223, and closed during non-selected period. Thus, electrodes, etc. are disposed to enable 1/3 time division driving, and the electrode shape of the liquid crystal panel is determined to a specified shape.

Description

【発明の詳細な説明】 不発明は液晶ライトバルブに関するものである。[Detailed description of the invention] The invention relates to a liquid crystal light valve.

最近の・rsw処理技術の進すは目ざましいものがあり
、それに伴ない例えばその出力装置の1つである印写装
置に対し、高@度、高速性が要求されている。さらに、
印写品位に対する要求も瓢く、これ會満址する印写装置
として、電子写巣と光蕾き込み音用いたレーザービーム
プリンタ(LBP、)あるいに光フアイバ管(OFT)
プリンタが実用に供されている。しかしながら上記のご
とく強い要求があるにもか刀Sわらず、LBP 、OF
T共に非常に高価なことが、普及を防げる大きな原因と
なっている。
Recent progress in RSW processing technology has been remarkable, and as a result, a printing device, which is one of its output devices, is required to have high performance and high speed. moreover,
Printing devices that meet the requirements for printing quality include laser beam printers (LBP) and optical fiber tubes (OFT) that use electronic photofocus and light buds.
The printer is in practical use. However, despite the strong demands mentioned above, LBP, OF
The fact that both T and T are extremely expensive is a major reason for preventing their widespread use.

本発明ニ、′D′−カる状況ケふまえ、従来アイデアの
みで、技術上の桓々の問題から実用化が困難とされてき
た液晶ライトバルブ方式の印写装置’に!現するために
、隔分# tiF4 、高品位、高速の光暑き込ユニツ
lf簡単な構成で、小型安価に提供することにある。
The present invention is directed to a liquid crystal light valve type printing device, which has been thought to be difficult to put into practical use due to numerous technical problems, even though it was only an idea in the past! In order to achieve this goal, the objective is to provide an interval #tiF4, high-quality, high-speed optical heating unit LF with a simple configuration, small size, and low cost.

液晶ライトバルブを含めた光吾込ユニットの構成上1図
に示す。光書込ユニットニけい光ランフ寺の光源用と液
晶ライトバルブ及び結像レンズ115刀1ら成す、液晶
ライトバルブに、液晶パネル、112と液晶駆動回路1
13を実装した基鈑114から成る。光源刀1ら出た光
に、液晶ライトバルブにより変調される。この元信号1
16は結像レンズ115により感光ドラム102上に結
像される、結像レンズには集束性光ファイバアレイ音用
いることによって正立像が得られる。第2図及び第3図
に液晶パネルの構成を示す。液晶パネルは、共通信号電
極119及び120?]l−備えるガラス基板117と
信号電極121及び122ケ備えるガラス基板118及
びスペーサー126の間に液晶組by、#125’z封
入したつ、カラス基板の両側に、偏光板123及び12
4ケ備えて成る。
Figure 1 shows the configuration of the Kogokomi unit including the liquid crystal light valve. The optical writing unit consists of a light source for a fluorescent light source, a liquid crystal light valve, and an imaging lens 115, a liquid crystal light valve, a liquid crystal panel, 112, and a liquid crystal drive circuit 1.
13 is mounted on the base plate 114. The light emitted from the light source sword 1 is modulated by a liquid crystal light valve. This original signal 1
An image 16 is formed on the photosensitive drum 102 by an imaging lens 115. An erect image is obtained by using a convergent optical fiber array sound for the imaging lens. FIGS. 2 and 3 show the structure of the liquid crystal panel. The liquid crystal panel has common signal electrodes 119 and 120? ] A liquid crystal assembly by #125'z is sealed between the glass substrate 117 provided with the signal electrodes 121 and 122 and the spacer 126, and polarizing plates 123 and 12 are placed on both sides of the glass substrate.
It consists of 4 pieces.

共通信号電極に、透明電極119と光学的に不透明な金
属電極120から成り、信号電極121及び122は透
明電極である。偏光板125と124は互いに偏光■が
直交するように配置されている。
The common signal electrode consists of a transparent electrode 119 and an optically opaque metal electrode 120, and the signal electrodes 121 and 122 are transparent electrodes. The polarizing plates 125 and 124 are arranged so that the polarized light (1) is orthogonal to each other.

光に共通電極の透明部分119と信号電極とで形成され
るマイクロシャッターの部分でKNされる、液晶組成物
として特願昭55−141085表1のネマチック液晶
に光学活性物質A−(2−metbylbulyl )
 −1’ −cyanobiphθnyls ’z 3
重量%疵加して得られた長周期コレステリック液晶を用
いることによって高速の液晶ライトパルプ會得ることが
できる。この液晶の訪電位万性の同波数特性′に第4図
に示す。誘電異万注がゼロである周波数を父差周波数と
呼びfcで表わす、fcより低い周波数忙fL、高い@
U波数τfHとする。このfLとfHの周波数の信号を
各信号電極に印加することによって、液晶ライトバルブ
は動作する。
The optically active substance A-(2-metbylbulyl )
-1' -cyanobiphθnyls 'z 3
By using the long-period cholesteric liquid crystal obtained by weight percent modification, a high-speed liquid crystal light pulp can be obtained. Figure 4 shows the same wave number characteristic of the universal potential of this liquid crystal. The frequency at which the dielectric difference is zero is called the difference frequency and is expressed by fc.
Let the U wave number be τfH. The liquid crystal light valve operates by applying signals of frequencies fL and fH to each signal electrode.

第5図(b)に印加信号と(a)液晶ライトバルブ’に
4遇した光の応答上*す。T2で示した時間fHの信号
、T3の時間fLの信号が印加されている。
Figure 5(b) shows the response of the applied signal and (a) the light incident on the liquid crystal light valve. A signal at time fH indicated by T2 and a signal at time fL at T3 are applied.

TI′に誓き込み周期、T2を開口時間、T5’f−非
開口時間と呼ぶ。fHの信号ケ印訓することによV液晶
ライトバルブに開き、fLの信号により閉じる、上述し
た方法により画期的に高速な液晶ライトパルプ上寿るこ
とができた、し刀1し高品印の印写を行なうために、マ
イクロシャッターf 1 mあたり10個程区の筒密度
に配置する必資がありA4版に印写するため幅20釧に
亜べなくてにならないためマイクロシャッターの数は2
000i[fflになる。このため上述した方法では、
信号電極のgに2000本さらに駆動回路及びこの実装
端子も2000個及び2000本になり、製作上歩留も
低下し、さらにコストが高くなる欠点があった。
TI' is called the commitment period, T2 is called the opening time, and T5'f is called the non-opening time. The V liquid crystal light valve opens by applying the fH signal and closes by the fL signal.By using the method described above, we were able to produce a revolutionary high-speed liquid crystal light pulp. In order to perform printing, it is necessary to arrange microshutters at a density of about 10 microshutters per meter, and in order to print on A4 size paper, it is necessary to reduce the width to 20mm, so the number of microshutters is 2
Becomes 000i[ffl. Therefore, in the method described above,
There are 2,000 signal electrodes per g, and 2,000 drive circuits and 2,000 terminals to mount the signal electrodes, resulting in lower production yields and higher costs.

従ってコストの低減をはかるために時分割駆動が提案さ
れているが、本発明でに弛時分割駆動全笑現するだめの
液晶パネルヶ提供スル。
Therefore, time-division driving has been proposed in order to reduce costs, but the present invention does not provide a liquid crystal panel that fully realizes time-division driving.

1ず偽時分割駆動法について1■単に述べる。第6図、
第7図に偽時分割の電極と、駆動波形を示す、、3つの
共通電憔2Q1,202.2[]3にそれぞれ選択信号
221.222,223會印加し信号電極205に、書
込みのデータに応じて開信号225又は閉信号226荀
印加する。この時、選択信号221〜224と開信号2
25、閉信号226は互いに逆位相である。、T1は副
走査周期、Taは選択期間、T’bに非選択期間であジ
、マイクロシャツ4−211〜213にそれぞれ選択信
号221〜223の選択期間に信号電極に加わる信号に
応じて開閉し、非選択の期間に閉じている。
1. The pseudo time-division driving method will be briefly described. Figure 6,
FIG. 7 shows the false time-division electrodes and drive waveforms. Selection signals 221, 222, 223 are applied to the three common voltages 2Q1, 202.2[]3, respectively, and the data to be written is applied to the signal electrode 205. An open signal 225 or a close signal 226 is applied depending on the condition. At this time, selection signals 221 to 224 and open signal 2
25, the close signals 226 are in opposite phase to each other. , T1 is the sub-scanning period, Ta is the selection period, and T'b is the non-selection period. and closed during non-selection periods.

第8図にこの様子會示した。イ■号電惟205に235
のような信号を加えた時、各マイクロシャッター211
〜213の光応答會231〜234にボした。以上の如
く狛時分割駆動が実現できたことによって大幅なコスト
ダウンが夾現できfc、。
Figure 8 shows this situation. I ■ No. 205 to 235
When a signal such as is applied, each micro shutter 211
I skipped the photo response sessions 231-234 of ~213. By realizing the continuous time-division drive as described above, a significant cost reduction can be realized.

しかし時分割の分割数が増えるにつれて信号′電極数が
減少するが、−万電極形状は複雑になる傾向がある。と
いうのは液晶ライトバルブにおいてにマイクロシャッタ
ー以外の部分での光漏れにすべてコントラストの低下に
なるため許されない。しかし第6図に示した如く共通電
極間のすき間と、信号電極間のすき間に必らず光漏れの
部分ができる。これ會実用土い刀1に小さくするかとい
うことが1つのポイントとなる。
However, as the number of time divisions increases, the number of signal electrodes decreases, but the shape of the electrodes tends to become more complex. This is not acceptable in a liquid crystal light valve because any light leakage in areas other than the microshutter will result in a decrease in contrast. However, as shown in FIG. 6, light leakage inevitably occurs in the gaps between the common electrodes and the gaps between the signal electrodes. One of the points is whether to reduce the size to 1 for practical use.

次にマイクロシャッター間の最大距離(第6図において
ぼ211と213のたて方間の距離〕が結像レンズとし
て使用する、集束性ファイバープレイによって制限され
る。といつのに本発明のように純炭f?行う場合、果収
注ファイバーレンズアレイでは、光軸力為らある距離以
上ずれると像の光電がいちじるしく低下する刀・らであ
る、筐た、一般に不発明のような大面積の微細パターン
に位置合わせの容易さ、マージン等が歩M’E9に大き
く影響する。
Next, the maximum distance between the microshutters (the distance between the vertical lines 211 and 213 in FIG. 6) is limited by the focusing fiber play used as the imaging lens. When using pure carbon fiber lens arrays, the optical axis force causes the photoelectricity of the image to drop significantly if the optical axis is shifted by more than a certain distance. The ease of alignment, margin, etc. of the fine pattern greatly affect the step M'E9.

以上の事全考慮して製作した不発明による液晶パネルの
電似パターンを示す、、第9図に第1のガラスに形成さ
れた共通電極で、5つに分割されている。選択信号を顧
える共遡゛隠極は201〜205で、両側の共典電憾3
01,302はダミー電極である。斜紛都はN1等の金
属膜で、不透明層となっており、残りの311.312
,313゜314に透明′成極である。この透明部は第
6図のマイクロシャッター211〜213に対応するが
t極の製作上212に対応するマイクロシャッターの位
置が312,314の2種類ある。
FIG. 9 shows an electronic pattern of an inventive liquid crystal panel manufactured with all of the above considerations in mind.It is divided into five parts by a common electrode formed on the first glass. The co-recurrence poles considering the selection signal are 201 to 205, and the co-recurrence poles on both sides are 3.
01 and 302 are dummy electrodes. The oblique part is a metal film such as N1, which is an opaque layer, and the remaining 311.312
, 313° and 314 with transparent polarization. This transparent portion corresponds to the microshutters 211 to 213 in FIG. 6, but due to the manufacturing of the t-pole, there are two types of microshutter positions 312 and 314 corresponding to 212.

次に第2のガラスに形成された信号電極を第10図に示
す。信号電極205(ゲインターディジタルに配置され
ているので、電4vのピッチPJJ300μmであるが
、実装する際にμ600μη1ピッチであるため大幅に
実装の信頼性、少留りが同上した。
Next, FIG. 10 shows the signal electrode formed on the second glass. Since the signal electrode 205 (gainer digital) is arranged, the pitch PJJ of 4V is 300 μm, but when it is mounted, the pitch is μ600 μη1, which greatly improves the reliability of the mounting and the small amount of space required.

信号電極205のが1紛部は不透明な金鵜1慣であり、
透明電性511〜314が共通電極の、)11〜314
と対間して配置されマイクロシャッター會形成する。
The first part of the signal electrode 205 is made of opaque metal.
) 11 to 314, where the transparent conductors 511 to 314 are common electrodes
A micro-shutter is formed between the shutter and the shutter.

千鳥状に並んだマイクロシャッターのピッチP1は10
0μm1 マイクロシャッター間距離はそれぞれ11(
’311−312間)が33μrx、J、(311−3
14間)が233prn、j13(511313間ンが
267μmである。これに時分割駆動で!@込んだ時水
平方間の直線を形成するドツトがずれないための条件−
副走査周期T1.感光体の移動速度會vとしたとき、マ
イクロシャッター間の間隔J=(−十n)xTV、(m
=1.2,3.n−1,1,2=す紮満足する。ただし
T= 2m 気、 V = 5 Cm / Seeとし
た。
The pitch P1 of the micro shutters arranged in a staggered manner is 10.
0 μm1 The distance between micro shutters is 11 (
'311-312) is 33μrx, J, (311-3
14 interval) is 233prn, and j13 (511313 interval) is 267μm.Conditions for not shifting the dots forming a horizontal straight line when driving in time division!
Sub-scanning period T1. When the moving speed of the photoreceptor is v, the interval between the microshutters J = (-10n) x TV, (m
=1.2,3. n-1, 1, 2 = Satisfied. However, T = 2m air and V = 5 cm/see.

以上の2枚のガラス?+4ねたものが第11図である。More than two pieces of glass? Figure 11 shows the +4 net.

電極ケ有する面どおしを重ねるのであるから、実際は第
9図か第10図のどちら刀・に鏡像である。
Since the surfaces with electrodes are overlapped, it is actually a mirror image of either Figure 9 or Figure 10.

第11図に示す如く、斜線都は丁べて不透明であるため
液晶パネルに入射した九はマイクロシャッター311〜
314でf、調され光誉込1g号となる。また光−れ部
321〜32ルからは常に光が漏れているので、光1g
号というm1点71>ら見るとオフセットニなる。征っ
てこのオフセットが谷マイクロシャッター間でばらつ刀
1ないエラに、マイクロシャッター211〜214と1
対1で対応するように、光漏れ部321〜324會配置
した、−万このオフセット分の量を実用上問題にならな
い根囲に抑えるために、光漏れ部の大きさt最/J%線
幅の10μm×10μmとした。実際この?願g量は、
マイクロシャッターの大きさ會100μm×90μmと
すると、デユーティ−?狛としても、3%にす゛ぎない
。−万製造歩留筐ジ會考慮して、最小線幅の、のべ長さ
?できるだけ小さくするために、光漏れを起こす部分の
近傍だけt最小線幅とした。
As shown in Fig. 11, since the shaded area is entirely opaque, the light incident on the liquid crystal panel is from the micro shutter 311 to
At 314, it is adjusted to f and becomes Mitsuyoshi-gomi 1g. Also, since light is always leaking from the light beams 321 and 32, 1g of light
If we look at the m1 point 71>, we get an offset ni. This offset is distributed between the valley micro-shutters, and the micro-shutters 211 to 214 and 1
The light leakage parts 321 to 324 are arranged so as to correspond to each other on a one-to-one basis. The width was 10 μm×10 μm. Actually this? The desired amount of g is
If the size of the microshutter is 100 μm x 90 μm, the duty? Even as a guardian, it's only 3%. - Considering the manufacturing yield of 10,000 yen, what is the total length of the minimum line width? In order to make it as small as possible, the minimum line width t was set only in the vicinity of the portion where light leakage occurs.

以上の如く本発明による液晶)(ネルの電極形状により
、狛時分割駆動の液晶)くネルを作ること75玉できた
。これにより高性能、低価格の光誉込ユニットを提供で
きる液晶ライトノ(ルブを構I戊することができた、
As described above, 75 pieces of the liquid crystal according to the present invention (liquid crystal driven in continuous time division due to the shape of the electrodes of the liquid crystal) were made. As a result, we were able to create a liquid crystal light system that can provide high-performance, low-cost light-included units.

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

第1図ぼ光蓄込信号発生部である。第2図、第3凶は液
晶パネルの構造を示した、第4図は本発明で用いた液晶
材料の蒋電異方注の周波数特注r示した図である、第5
図は本発明に使用した液晶材料の応答特注及びその時の
駆動信号上水した図である。 第6図、第7図は始時分割電極構造の原理図と駆動信号
波形7示した。 第8図il″I弛時分割駆動時の谷マイクロシャッター
の光レスポンスと駆動波形デポした。 第9図、第10図は本発明である液晶パネルの第1のガ
ラスと第2のガラスの電体形状會示した。 第11図は、2枚のガラスを車ねた時の電極形状を示し
た、 201%2Q3・・・共通電極 205・・・信号電極 211〜214,311〜314・・・マイクロシャッ
ター321〜624・・・光重れ部 第1図 t4 第2図 第3図 第4図 第5図 cx  rLrLf’L二■面几/22 ZC13m川
コ■−用A−/Zz口 第7図 第8図 第9ト[1 第10図
FIG. 1 shows a light accumulation signal generating section. Figures 2 and 3 show the structure of the liquid crystal panel, Figure 4 shows the frequency custom made by Chiang Dian Anifang of the liquid crystal material used in the present invention, and Figure 5 shows the structure of the liquid crystal panel.
The figure is a diagram showing the custom response of the liquid crystal material used in the present invention and the driving signal at that time. FIGS. 6 and 7 show the principle diagram of the starting time division electrode structure and the drive signal waveform 7. Figure 8 shows the optical response and drive waveform of the valley microshutter during relaxation time-division driving. Figure 11 shows the shape of the electrodes when two pieces of glass are connected. 201%2Q3...Common electrode 205...Signal electrodes 211-214, 311-314...・Micro shutter 321 to 624...Light overlapping part Fig. 1 t4 Fig. 2 Fig. 3 Fig. 4 Fig. 5 cx rLrLf'L two-face box/22 A-/Zz mouth for ZC13m river co- Figure 7 Figure 8 Figure 9 [1 Figure 10

Claims (1)

【特許請求の範囲】 [1)  L/sの時分割駆動される液晶ライトバルブ
において、液晶パネルが、少なくとも3つに分割された
共通電極’r−”Mする第1のガラスと、分割された共
通電極のすき間七父差対向する部分が不適切である部分
?有する複数個の信号電極葡有する絹2のガラスからな
り、該第1.第2のガラスは交差対向するように配置さ
れ、その間に常温で該電異万性が零となる交差周波数f
cが100KHz以上であるネマチック液晶に光学活性
物質全添加してなる液晶材料上封入したこと’に%憾と
する液晶ライトバルブ。 (2)該液晶パネルにおいて、該共通電惨と該4g号電
極によって構成されるマイクロシャッターは千鳥状に配
列され、その間崗が、副走宜周期盆Tl感光体の移動速
度2vとしだ時(−+n )xT、xV(m=1.2.
3・n=、0,1.2・・・)で与えられること全特徴
とする特許請求の範囲第1項記載の液晶ライトバルブ。 (3)  該マイクロシャッター以外の光副れ部の面積
カ該マイクロシャッターに比べて十分小さく、刀為つ、
該マイクロシャッターと該光漏れ部が1対1に対応して
いること全特徴とする特許請求の範囲第1項記載の液晶
ライトバルブ。 (4)少なくとも該光漏れ部の近傍の電極パターンが、
該液晶パネルの最小線幅であること全特徴とする特許請
求の範囲第1項記載の液晶ライトバルブ。
[Scope of Claims] [1] In a liquid crystal light valve driven in L/s time division, the liquid crystal panel is divided into a first glass having a common electrode 'r-''M divided into at least three parts, The signal electrode is made of silk glass having a plurality of signal electrodes having a gap between the common electrodes and the opposing portions are inappropriate, and the first and second glasses are arranged to cross each other, and In the meantime, the cross frequency f at which the electrical anisotropy becomes zero at room temperature
We regret that the liquid crystal light valve is encapsulated on a liquid crystal material made by adding all optically active substances to a nematic liquid crystal whose c is 100 KHz or more. (2) In the liquid crystal panel, the microshutters constituted by the common electric current and the No. 4g electrode are arranged in a staggered manner, and when the movement speed of the secondary periodic tray Tl photoreceptor reaches 2v, the microshutters are arranged in a staggered manner. -+n)xT,xV(m=1.2.
3.n=, 0, 1.2...) The liquid crystal light valve according to claim 1, wherein all the characteristics are given by: (3) The area of the light secondary portion other than the micro-shutter is sufficiently small compared to the micro-shutter;
2. The liquid crystal light valve according to claim 1, wherein the micro shutter and the light leakage portion have a one-to-one correspondence. (4) At least the electrode pattern near the light leakage portion is
The liquid crystal light valve according to claim 1, characterized in that the liquid crystal panel has a minimum line width.
JP58004587A 1983-01-14 1983-01-14 Liquid crystal light valve Pending JPS59128518A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58004587A JPS59128518A (en) 1983-01-14 1983-01-14 Liquid crystal light valve

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58004587A JPS59128518A (en) 1983-01-14 1983-01-14 Liquid crystal light valve

Publications (1)

Publication Number Publication Date
JPS59128518A true JPS59128518A (en) 1984-07-24

Family

ID=11588165

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58004587A Pending JPS59128518A (en) 1983-01-14 1983-01-14 Liquid crystal light valve

Country Status (1)

Country Link
JP (1) JPS59128518A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2569871A1 (en) * 1984-08-31 1986-03-07 Casio Computer Co Ltd RECORDING CONTROL METHOD

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2569871A1 (en) * 1984-08-31 1986-03-07 Casio Computer Co Ltd RECORDING CONTROL METHOD

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