JPS59119319A - Liquid crystal light valve - Google Patents

Liquid crystal light valve

Info

Publication number
JPS59119319A
JPS59119319A JP57228942A JP22894282A JPS59119319A JP S59119319 A JPS59119319 A JP S59119319A JP 57228942 A JP57228942 A JP 57228942A JP 22894282 A JP22894282 A JP 22894282A JP S59119319 A JPS59119319 A JP S59119319A
Authority
JP
Japan
Prior art keywords
liquid crystal
light valve
signal electrodes
micro
light
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
JP57228942A
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 JP57228942A priority Critical patent/JPS59119319A/en
Publication of JPS59119319A publication Critical patent/JPS59119319A/en
Pending legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B41PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
    • B41JTYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
    • B41J2/00Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
    • B41J2/435Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective application of radiation to a printing material or impression-transfer material
    • B41J2/465Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective application of radiation to a printing material or impression-transfer material using masks, e.g. light-switching masks

Landscapes

  • Liquid Crystal (AREA)
  • Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)

Abstract

PURPOSE:To obtain a high-resolution, high-quality, and high-speed optical writing unit of simple constitution by charging prescribed liquid crystal between a couple of glass substrates which have four split common signal electrodes and plural signal electrodes. CONSTITUTION:A liquid crystal panel consists of a glass substrate 117 equipped with common signal electrodes 119 and 120, a glass substrate 118 equipped with signal electrodes 121 and 122, a spacer 126, and a liquid crystal composition 125, and has polarizing plates 123 and 124 at right angles. The signal electrodes 121 and 122 are transparent electrodes. Light is modulated at the part of the microshutter consisting of a transparent part 119 and the signal electrodes 121 and 122 and then written. An optical active material is added to cholesteric liquid crystal of >=100kHz in cross frequency for the liquid crystal composition 125 to obtain the high-speed light valve. Thus, the high-resolution, high-quality, and high-speed optical writing operation is performed through the simple constitution by 1/4 time division driving.

Description

【発明の詳細な説明】 本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 present invention relates to a liquid crystal light valve.

最近の情報処理技術の進歩は目ざましいものがあり、そ
れに伴々い例えばその出力装置の1・りである印字装置
に対し、高密度、高速性が要求されている。ζらに、印
写品位に対する要求も強く、これを満足する印写装置と
しで、電子写真と光書き込みを用いたレーザービームプ
リンタ(LBP)あるいけ光フアイバ管(02丁)プリ
ンタが実用に供されていZ・。しかしながら上目1′の
ごとく強い要求があるにもかかわらず、LBF、’OF
T共に非常に高価方ことが、普及を防げる大き々原因と
なっている。
Recent advances in information processing technology have been remarkable, and along with this, high-density and high-speed performance are required of printing devices, which are one of the output devices. ζ and others have strong demands for printing quality, and laser beam printers (LBPs) and optical fiber tube (02) printers that use electrophotography and optical writing have been put into practical use as printing devices that satisfy these demands. It has been Z. However, despite strong demands as mentioned in item 1', LBF, 'OF
The fact that both T and T are extremely expensive is a major reason why they have not become popular.

本発明は、かかる状況をふまえ、従来アイデアのみで、
技術上の種々の問題から実用化が困齢とされてきた液晶
ライトバルブ方式の印字装置6を実現するために、高分
解能、高品位、高速の光V!き込ユニットを簡単な構成
で、小型安価に提供することにある。
In view of this situation, the present invention was developed using only conventional ideas.
In order to realize the liquid crystal light valve type printing device 6, which has been considered difficult to put into practical use due to various technical problems, we developed a high-resolution, high-quality, high-speed optical V! To provide a small and inexpensive loading unit with a simple configuration.

液晶ライトバルブを含めた光杏込ユニットの構成を第1
図に示す。光誉込ユニットははい光ランプ等の光源用と
液晶ライトバルブ及び結像レンズ115から成り、液晶
ライトバルブハ、液晶パネル、112と液晶駆動回1i
113ff実砦し1c基板114から成る7光源から出
た光は、液晶ライトバルブにより変調される。この光信
遅116は結像レンズ115により感光ドラム102上
に結像これる。結像レンズには集束性光ファイバアレイ
を用いることによって正立像が得られる。、筐2図及び
第3図に液晶パネルの横加を示す、、′0晶/シネルは
、共通信呆電極119及び120を備えるガラス基板1
17と信妥電極121及び122を備えるガラス基板1
18及びスペーサー126の間に液晶組成物125を封
入しかつ、ガラス基板の両側に、偏光飯123及び12
4を備えで威る。
First, the configuration of the optical unit including the liquid crystal light valve.
As shown in the figure. The optical unit consists of a light source such as a light lamp, a liquid crystal light valve, and an imaging lens 115, and includes a liquid crystal light valve, a liquid crystal panel, 112, and a liquid crystal drive circuit 1i.
Light emitted from seven light sources consisting of a 113FF and 1C substrate 114 is modulated by a liquid crystal light valve. This optical signal 116 is imaged onto the photosensitive drum 102 by the imaging lens 115. An erect image can be obtained by using a focusing optical fiber array as the imaging lens. , Figure 2 and Figure 3 show the horizontal mounting of the liquid crystal panel.
17 and a glass substrate 1 comprising reliable electrodes 121 and 122
A liquid crystal composition 125 is sealed between 18 and a spacer 126, and polarized films 123 and 12 are placed on both sides of the glass substrate.
Be prepared for 4.

共通信畳電極は、透明電極119と光学的に不透明か金
属電極120から成り、信芸電極121及び122け透
明電極である641M光板123と124は互いに偏光
面が直交するように配置されている。光は共通電極の透
明部分119と信号電極とで形成されるマイクロシャッ
ターの部分で変調される。液晶組放物として特願昭55
−14’1085表1のネマキツ々液晶に光学活性物’
Ji 4−(2−methylbulyl ) −4’
 −cyan。
The Kyodo Tatami electrode consists of a transparent electrode 119 and an optically opaque metal electrode 120, and the 641M light plates 123 and 124, which are the transparent electrodes of the Shingei electrodes 121 and 122, are arranged so that their polarization planes are orthogonal to each other. . The light is modulated by the micro-shutter formed by the transparent portion 119 of the common electrode and the signal electrode. Patent application filed in 1984 as a liquid crystal paraboloid
-14'1085 Optically active substances in the liquid crystals shown in Table 1
Ji 4-(2-methylbulyl)-4'
-cyan.

−bip、henyls  を6重量係添加して得られ
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
の液晶ライトバルブを得ることができる。この液晶の線
電位方性の周波敬特性fy4図に示す。
A high-speed liquid crystal light valve can be obtained by using a long-period cholesteric liquid crystal obtained by adding 6 parts by weight of -bip, henyls. The frequency characteristic of the line potential sotropy of this liquid crystal is shown in Fig. fy4.

誘電異方性がゼロである周波数を父差周波敬と呼びfc
で表わす。fcより低い周波数をfL、高い周波数ff
Hとする。このfLとfHの周波数の信呆を各信号電極
に印加することによって、液晶ライトバルブは動作する
。第5図(b)に印加信芸と(a) !晶うイトバルブ
を透過した光の応答を示す。
The frequency at which the dielectric anisotropy is zero is called the differential frequency fc
It is expressed as The frequency lower than fc is fL, the higher frequency ff
Let it be H. The liquid crystal light valve operates by applying frequencies of fL and fH to each signal electrode. Figure 5 (b) is applied to Shingei and (a)! This shows the response of light transmitted through a crystal light bulb.

T2で示′した時間fHの信ぜ、T6の時間fLの信号
が印加されている。T1を葬き込み周期。
A signal at time fH indicated by T2 and a signal at time fL at T6 are applied. A cycle that incorporates T1.

T2を開口時間、T6?非開ロ詩間と呼ぶ。fHの信号
を印加することにより液晶ライト1バルブは開き、fL
の信呆により閉じる、上述した方法により画期的に高速
な液晶ライトバルブを得ることができた。しかし高品印
の印写を行方うために、マイクロシャッターを1咽あた
り10個程度の高密度に配置する必要があり、A4版に
印写する1ζめ幅20ctnに並らべh(てはhらない
ためマイクロシャッターの斂は2000個になる。この
ため上述した方法では、信号電極の藪は2000本さら
に駆動回路及びこの実装端子も2000個及び2000
木に方り、製作上歩留も低下し、さらにコストが高(な
る欠点があった。
T2 is the opening time, T6? It is called Shima, which is not open to the public. By applying the fH signal, the liquid crystal light 1 bulb opens, and the fL
With this confidence, we were able to obtain a revolutionary high-speed liquid crystal light valve using the method described above. However, in order to print a high-quality seal, it is necessary to arrange microshutters at a high density of about 10 per hole, and they are lined up in a width of 20ctn on the 1ζ scale to be printed on an A4 plate. Therefore, in the method described above, there are 2,000 signal electrodes and 2,000 drive circuits and their mounting terminals.
The disadvantage was that the wood was too thin, the manufacturing yield was low, and the cost was high.

従ってコストの低減をはかるために時分割駆動が粉案さ
れているが、本発明ではμ時分割駆動を実現するための
液晶パネルを提供する。
Therefore, time-division driving has been proposed in order to reduce costs, and the present invention provides a liquid crystal panel for realizing μ time-division driving.

甘ずl74UFP分割駆動法について簡単に述べる。第
6図1.第7図にV4時分割の電極と、駆動波形を示す
、%4つの共通電極201,202,203゜204に
それぞハ選択信号22i、222゜223.224f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を印加する。この時選択信号
221〜224と開信号2251閉信呆226(l−を
互いに逆位相である。T1は副走査周期、Taけ選択期
間、Til”i:1IliF選択期間であり、マイクロ
シャッター211〜214けそれぞれ選択信号221〜
224の選択期間に信呆電極に加わる信号に応じて開閉
し、非選択の期間は閉じている。第8り1にこの様半を
示した、信号電極205に235のような信号を加えた
時、各マイクロシャッタ211214の光応答を231
〜264に示した。以上の如(μ時分割駆動が実現でき
たことによって大幅方コストダウンが実現できた。
Amazu 174UFP split driving method will be briefly described. Figure 6 1. FIG. 7 shows the V4 time-division electrodes and drive waveforms.C selection signals 22i, 222°223.224f are applied to the four common electrodes 201, 202, 203°204, respectively, and writing is performed on the signal electrode 205. An open signal 225 or a close signal 226 is applied depending on the data. At this time, the selection signals 221 to 224 and the open signal 2251 close signal 226 (l- are in opposite phases to each other. T1 is the sub-scanning period, Ta selection period, Til"i:1IliF selection period, and the micro shutter 211 to 214 selection signals 221~
It opens and closes in response to the signal applied to the signal electrode during the selection period of 224, and remains closed during the non-selection period. This situation is shown in Part 8. When a signal like 235 is applied to the signal electrode 205, the optical response of each micro-shutter 211214 is 231.
~264. As described above, by realizing μ time-division driving, a significant cost reduction was achieved.

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、一方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はマイクロシャッター
以外の部分での光漏れはすべてコントラストの低下にな
るため許され々い。
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 because in a liquid crystal light valve, any light leakage from any part other than the microshutter is unacceptable because it will reduce the contrast.

(、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ず光漏れの部分ができる。
(However, as shown in FIG. 6, light leakage always occurs in the gaps between the common electrodes and the gaps between the signal electrodes.

これを実用上いかに小さくするかということが。The question is how to make this small in practical terms.

1つのポイントとなる。This is one point.

次ニマイクロシャッター間の最大比1171 (第6 
図においては211と214のたて方向の距離)が。
The maximum ratio between the second and second microshutters is 1171 (6th
In the figure, the distance between 211 and 214 in the vertical direction) is.

結像レンズとして使用する、集束性ファイバープレイに
工って制限される。というのは本発明のように線走査を
行う場合、集収性ファイバーレンズアレイでは、光軸か
らある距離以上ずれると像の光量がいちじるしく低下す
るからとある。
Limited to a focusing fiber play for use as an imaging lens. This is because when line scanning is performed as in the present invention, the amount of light in the image decreases significantly when the focusing fiber lens array deviates from the optical axis by more than a certain distance.

また一般に本発明のような大Ifi積の微細ノくターン
は位置合わせの容易さ、マージン面が歩留tりに大きく
影響する。
Furthermore, in general, in the case of fine turns with a large Ifi product as in the present invention, the ease of alignment and the margin surface greatly affect the yield t.

以上の裏を考慮して製放した本発明による液晶パネルの
電極パ〃−ンを第9図に示す。(a) Id第1のガラ
スに形成きれた共通電極で、6つに分割されている。選
択信号を加える共通電極け201〜204で1画伺1の
共通電極301.302けダミー屯榛である。各共通電
極ではマイクロシャッター211〜214の部分が透明
電極であり、残りの斜線部は不透明々Ni%の金属電極
でできている。
FIG. 9 shows the electrode pattern of a liquid crystal panel according to the present invention, which was manufactured with the above considerations in mind. (a) Id is a common electrode completely formed on the first glass, and is divided into six parts. The common electrodes 201 to 204 to which selection signals are applied are dummy electrodes 301 and 302, each having a width of 1. In each common electrode, the portions of the microshutters 211 to 214 are transparent electrodes, and the remaining hatched portions are made of opaque Ni% metal electrodes.

千鳥状に並んだマイクロシャッターのピッチP1け10
0μm、マイクロシャッター間圧はそれぞれ/’s (
211−212間)が25μm。
Pitch of micro-shutters arranged in a staggered pattern P1 to 10
0μm, microshutter pressure is /'s (
211-212) is 25 μm.

/5(211213間)が450μm−es (211
−214間)が475μmである。これは時分割駆動で
婁き込んで時水半方向の直線を形成するドツトがずわ方
いための条件−副走査周期+T1.感光体の移動速度y
vとしたとき、マイクロシャッター間の間’RFse=
(−+n)XTV  (tn=1゜2.6・n=+0+
1+2・・・)を満足する。ただしT = 2 mx、
 V = 5 cm/stxとした。
/5 (between 211213) is 450μm-es (211
-214) is 475 μm. This is a condition for the number of dots that are intersected by time-division driving to form a straight line in the half-time direction - sub-scanning period + T1. Photoconductor moving speed y
When v, the interval between the microshutters 'RFse=
(-+n)XTV (tn=1゜2.6・n=+0+
1+2...) is satisfied. However, T = 2 mx,
V = 5 cm/stx.

次にv、2のガラスに形繍享ねた信秘区極を(b)に示
す、信号電極205け斜線部が金属膜で不透明であり、
それ以外611が透明電極である。電極端子間ピ”’−
Pg ilt 400 prn f、20σT500本
ある6ドライバーエCに実装する時、400μmピッチ
であるのでそれほどの畑かしさけないが、信号電極端子
をインターディジタルに配置すわば、片側のピッチが8
00μm トfx リ。
Next, (b) shows the secret area embossed on the glass of v.2, where the shaded area of the signal electrode 205 is made of a metal film and is opaque.
The other part 611 is a transparent electrode. Pin between electrode terminals
Pg ilt 400 prn f, 20σT When mounting on a 6-driver E-C with 500 wires, the pitch is 400 μm, so it will not take much effort, but if the signal electrode terminals are arranged interdigitally, the pitch on one side will be 8.
00μm Tofx Li.

さらに実装が容易と々る。Furthermore, it is easy to implement.

以上の2枚のガラスを重ねたものが第10図である。電
極を有する面どおしを重ねるのであるから、実際は筈9
図の(a)と(b)のどちらかは鋭像である。
FIG. 10 shows the above two glasses stacked together. Since the surfaces with electrodes are stacked on top of each other, it should actually be 9.
Either (a) or (b) of the figure is a sharp image.

第10し1に示す如(、斜線部はすべて不透明であるた
め、液晶パネルに入射した光はマイクロシャッター21
1〜214で浚−これ光書込信号と々る。また光漏れ部
421〜624からは常に光が漏ねているので、光信号
という観点から見るとオフセットにhる。従ってこのオ
フセットが各マイクロシャッター間でばらつかhい工う
に、マイカロシイツタ−211〜214と1対1で対応
するように、光漏れ部321〜624を配置した7一方
このオフセット分の量を実用上問題にたらない程度に抑
えるために、光漏れ部の大きさ全最小線幅の10μm×
10μmとした。実際この漏れ量は、マイクロシャッタ
ーの大きさを100μm×90pmとすると、デユー子
イを%とじても。
As shown in No. 10 and 1 (the shaded areas are all opaque, the light incident on the liquid crystal panel is transmitted to the micro shutter 21).
1 to 214, the optical write signal arrives. Furthermore, since light always leaks from the light leakage portions 421 to 624, this results in an offset from the perspective of an optical signal. Therefore, since this offset varies among the microshutters, the light leakage portions 321 to 624 are arranged so as to correspond one-to-one with the microshutters 211 to 214. On the other hand, the amount of this offset can be adjusted in practical terms. In order to keep it to a non-problematic level, the size of the light leakage part should be 10 μm x the total minimum line width.
It was set to 10 μm. In fact, if the size of the microshutter is 100 μm x 90 pm, this amount of leakage will be calculated even if the amount of leakage is reduced by %.

4係にすぎ々い。一方製造歩留祉りを考慮して、最小線
幅ののべ長さをできるだけ小さくするために、光d1i
れを起こす部分の近傍だけを最小線幅としたー 以上の如く本発明による液晶パネルの電極形状により、
μ時分割駆動の液晶パネルを作ることができた。こねに
エリ高性能、低価格の光p、込ユニットを提供できる液
晶ライトバルブを構成することができた、
There are too many people in charge 4. On the other hand, in consideration of manufacturing yield, in order to minimize the total length of the minimum line width, the optical d1i
With the electrode shape of the liquid crystal panel according to the present invention as described above, the line width is minimized only in the vicinity of the part where the distortion occurs.
We were able to create a μ time division driven liquid crystal panel. We were able to construct a liquid crystal light valve that can provide a high-performance, low-cost optical unit.

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

第1図は光書迷信≠発生部である。第2図、笹3図は4
ゲ晶パネルの構造を示した。]ゝ:4−は本発明で用い
た液晶材料の誘屯異方件の周波斂特性を示した一である
。第5関は本発明に使用した液晶材料の応答特性及びそ
の時の駆動信号を示した図である。 第6図,第7図rl′iV4晴分割電極構遺の原理図と
駆動化量波形を示した・ 第8図は%時分制勝・励時の各マイクロシャッターの光
レスポンスと駆動波形を示した。 第9図1 (a) (b)は本発明である液晶パネルの
第1のガラスと,第2のガラスの電極形状を示した。 第10邸1に、2枚のガラス?重ね1こ時の電極形状を
示した。 201〜204・・・・・・共通電接 205・・・・・・信芸区極 211〜214・・・・・・マイクロシャッター321
〜624・・・・・・光漏れ化 第2図 第3図 第5図 第6図 第 7 「°イ[ 〜イ)81 21+                  ・ 咬(
へ3゜I第′9図 3スλ 第10図
Figure 1 shows the origin of the light book superstition. Figure 2, bamboo grass 3 is 4
The structure of the crystal panel is shown. ]ゝ:4- is one showing the frequency convergence characteristics of the dielectric anisotropy of the liquid crystal material used in the present invention. The fifth section is a diagram showing the response characteristics of the liquid crystal material used in the present invention and the driving signal at that time. Figures 6 and 7 show the principle diagram and drive waveform of the rl'iV4 clear split electrode structure. Figure 8 shows the optical response and drive waveform of each microshutter during % time control and excitation. Ta. FIGS. 9(a) and 1(b) show the electrode shapes of the first glass and the second glass of the liquid crystal panel according to the present invention. Two pieces of glass in the 10th house 1? The shape of the electrode at the time of one stack is shown. 201-204... Common electrical connection 205... Shingei-ku pole 211-214... Micro shutter 321
~624...Light leakage Figure 2 Figure 3 Figure 5 Figure 6 Figure 7
To 3゜I Fig. '9 3 S λ Fig. 10

Claims (1)

【特許請求の範囲】 ■ μの時分制勝1Jibされる液晶ライトバルブにお
いて、 7pi晶パネルが、少なくとも4つに分割され
た共通電極を有する第1のガラスと1分例でねた共通電
極のすき間と交差対向する部分が不透明である部分を有
する複数個の信会電極を有する第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配置され、そ
の間に當温で誘雷、異方性が零と々る交差周波数fcが
100 KH2以上であるネマ千ツク液晶に光学活性物
質を添加してなる液晶材f−4全封入したことを特徴と
する液晶ライトバルブ。 ■ 該液晶パネルにおいて、該共通′区極と該信号電極
によって欅戚ζねるマイクロシャッターは千鳥状に配列
され、その間隔が、副走者周期をT+、感光体の移動速
度を■とした時(−+n )XTI  XV   (m
=11 21 3eH,=Q、11 2・・・)で与え
られることを特徴とする特許請求の範貯第1項言2転の
液晶ライトバルブ。 ■ 該マイクロシャッター服外の光漏h g ノ面1i
ft d” 該マイクロ7ヤツターに比べて子分小さく
。 カッ該マイクロシャッターと該光漏れ部が1対1に対応
していることを特徴とする特許請求の範囲第1項記載○
液晶ライトバルブ。 ■ 少りくとも該光漏れ部の近傍の電惨パターンが、該
液晶パネルの最小線幅であることを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] ■ In a liquid crystal light valve with a time division of μ, a 7pi crystal panel has a first glass having a common electrode divided into at least four parts and a common electrode having a common electrode divided into at least four parts. consisting of a second glass having a plurality of contact electrodes, each of which has an opaque portion that intersects with the gap;
Part 1. The second glasses are arranged so as to cross each other, and between them, an optically active material is added to a nematic liquid crystal whose cross frequency fc at which the anisotropy reaches zero is 100 KH2 or more and which is lightning-resistant at a temperature of 100 KH2. A liquid crystal light valve characterized by being completely filled with liquid crystal material F-4. ■ In the liquid crystal panel, the micro-shutters arranged in a staggered manner by the common electrode and the signal electrode are arranged in a staggered manner, and the interval between them is as follows: ( −+n ) XTI XV (m
=11 21 3eH, =Q, 11 2...) A liquid crystal light valve as set forth in claim 1. ■ Light leakage outside the micro-shutter clothing
ft d" is smaller than the Micro 7 Yator. Claim 1, characterized in that the micro shutter and the light leakage portion correspond one to one.○
LCD light bulb. (2) The liquid crystal light valve according to claim 1, wherein the electrical failure pattern at least near the light leakage portion has the minimum line width of the liquid crystal panel.
JP57228942A 1982-12-27 1982-12-27 Liquid crystal light valve Pending JPS59119319A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57228942A JPS59119319A (en) 1982-12-27 1982-12-27 Liquid crystal light valve

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57228942A JPS59119319A (en) 1982-12-27 1982-12-27 Liquid crystal light valve

Publications (1)

Publication Number Publication Date
JPS59119319A true JPS59119319A (en) 1984-07-10

Family

ID=16884261

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57228942A Pending JPS59119319A (en) 1982-12-27 1982-12-27 Liquid crystal light valve

Country Status (1)

Country Link
JP (1) JPS59119319A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5458664A (en) * 1992-05-13 1995-10-17 Sumitomo Electric Industries, Ltd. Particulate trap for purifying diesel engine exhaust
US7508478B2 (en) 2003-09-18 2009-03-24 Citizen Holdings Co., Ltd. Display apparatus

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5458664A (en) * 1992-05-13 1995-10-17 Sumitomo Electric Industries, Ltd. Particulate trap for purifying diesel engine exhaust
US7508478B2 (en) 2003-09-18 2009-03-24 Citizen Holdings Co., Ltd. Display apparatus

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