JPS62247329A - Liquid crystal display element - Google Patents

Liquid crystal display element

Info

Publication number
JPS62247329A
JPS62247329A JP60287410A JP28741085A JPS62247329A JP S62247329 A JPS62247329 A JP S62247329A JP 60287410 A JP60287410 A JP 60287410A JP 28741085 A JP28741085 A JP 28741085A JP S62247329 A JPS62247329 A JP S62247329A
Authority
JP
Japan
Prior art keywords
liquid crystal
electrode substrate
degrees
angle
polarizing plate
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
JP60287410A
Other languages
Japanese (ja)
Inventor
Chiyoaki Iijima
千代明 飯島
Keiji Wada
啓志 和田
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson 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 Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP60287410A priority Critical patent/JPS62247329A/en
Publication of JPS62247329A publication Critical patent/JPS62247329A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To improve time division driving characteristic by specifying angle of torsion, angle formed by light absorption axes or polarization axes of a pair of polarizing plates, and product of refractive index anisotropy and thickness of a liquid crystal layer. CONSTITUTION:An upper electrode substrate and a lower electrode substrate are arranged opposite to each other to make the direction 6 of rubbing of the upper electrode substrate nearly conform to liquid crystal molecule orientation and the direction 7 of rubbing of the lower electrode substrate nearly conform to liquid crystal molecule orientation and to make the direction and angle 10 of liquid crystal molecule in the range of above 200 deg.. On the other hand, the upper polarizing plates is placed on the outer face of the upper electrode substrate and the lower polarizing plate is placed on the outer face of the lower electrode substrate to make the angle 11 formed by the absorption axis 8 of the upper polarizing plate and absorption axis 9 of the lower polarizing plate within the range from 60 deg. to 120 deg.. It is desirable to make the product of refractive index anisotropy DELTAn of the liquid crystal and thickness (d) of the liquid crystal layer within the range from 0.2mum to 0.7mum. Thereby, sufficient contrast can be obtained in time division driving when duty ratio is less than 1/100.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は液晶表示素子に係わり、特に時分割特性を向上
させtツイストチットネマチック(TN)形液晶表示素
子に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a liquid crystal display element, and more particularly to a t-twist chit nematic (TN) type liquid crystal display element with improved time division characteristics.

〔従来の技術〕[Conventional technology]

一般に液晶表示装置において、2枚の電極基板間で液晶
分子がらせん状構造金なすように配向させるには、例え
ば゛電極基板の液晶に接触する表面を布などで一方向に
こする方法、いわゆるラビング法によってなされる。こ
のようにして配向処理され7t2枚の電極基板をそれぞ
れのラビング方向すなわち配向方向に例えば互いにほぼ
90度に交差する工うに対向させ、2枚の電極基板をシ
ール剤に工t)接涜し、その間隙に正の誘電異方性tも
つtネマチック液晶を封入すると、液晶分子はその電極
関金はぼ90[回転し九らせん状倉造の分子配列をする
In general, in a liquid crystal display device, in order to align the liquid crystal molecules between two electrode substrates so that they form a spiral structure, for example, there is a method called ``rubbing the surface of the electrode substrate that contacts the liquid crystal in one direction with a cloth, etc.'' It is done by rubbing method. The two electrode substrates that have been oriented in this way are placed facing each other in the rubbing direction, that is, the orientation direction, for example, in a manner that intersects each other at approximately 90 degrees, and the two electrode substrates are then exposed to a sealant. When a t-nematic liquid crystal having a positive dielectric anisotropy t is filled in the gap, the liquid crystal molecules rotate about 90° at the electrodes and form a nine-helical molecular arrangement.

このLうに構造されt液晶セルの上下には偏光板が設け
られるが、この偏光板の光吸収軸あるいは偏光軸は上下
2枚のt極基板のラビング方向にそれぞれほぼ一致して
いる。
Polarizing plates are provided above and below this L-shaped T liquid crystal cell, and the light absorption axis or polarization axis of the polarizing plates substantially coincides with the rubbing direction of the two upper and lower T-pole substrates, respectively.

第2図は前述しt従来のTN形液晶表示素子のラビング
方向と偏光板の軸との関・係についてモデル的に示し九
園である。同図において、1tl′i上側電極基板のラ
ビング方向、2は下側電極基板のラビング方向、5は上
側偏光板の光吸収軸あるいはイ:4光軸、4は下@偏光
板の光吸収’41あるいは偏光軸、5ri液晶分子のね
じれ方向お工び角変である。
FIG. 2 is a model showing the relationship between the rubbing direction of the conventional TN type liquid crystal display element and the axis of the polarizing plate as described above. In the figure, 1tl'i is the rubbing direction of the upper electrode substrate, 2 is the rubbing direction of the lower electrode substrate, 5 is the light absorption axis of the upper polarizing plate, or A: 4 optical axis, 4 is the lower @ light absorption of the polarizing plate. 41 or the polarization axis, 5ri is the twist direction of the liquid crystal molecules and the angle change.

このように構造され、6’l’N形液晶表示g;に置け
、近年、液晶表示装置の電気光学特性、特に時分割部r
iJ特性に対する要求度が厳しくなっており、このよう
な要求仕様に対して十分に1足できない状況に至ってい
る。
In recent years, electro-optical characteristics of liquid crystal display devices, especially in the time division section, have been developed.
Requirements for iJ characteristics are becoming stricter, and we have reached a situation where it is not possible to meet these required specifications.

〔発明が解決し:うとする問題点〕[Problems that the invention attempts to solve]

液晶表示装置において、デユティ比1/10G  以下
の低デユティmsになると、充分なコントラストが得ら
れず、問題となる。
In a liquid crystal display device, when the duty ratio is low (ms), such as a duty ratio of 1/10 G or less, sufficient contrast cannot be obtained, which poses a problem.

〔間頂点を解決する之めの子役〕[The child actor who solves the intervening vertices]

本発明の表示装置は、この工うに問題を解決する几めに
、液晶分子のねじれ内金200度以上の範囲とし、一対
の偏光板の光吸収軸あるいは偏光軸のなす角が60度か
ら120度までの範囲とし液晶の屈折率異方性△nと液
晶層の厚さd(μm)との積△ndが12μmから17
μmの範囲内にあること全特徴としている。
In order to solve this problem, in the display device of the present invention, the internal twist of the liquid crystal molecules is in the range of 200 degrees or more, and the angle between the light absorption axes or polarization axes of the pair of polarizing plates is from 60 degrees to 120 degrees. The product Δnd of the refractive index anisotropy Δn of the liquid crystal and the thickness d (μm) of the liquid crystal layer is from 12 μm to 17
All characteristics are that it is within the μm range.

〔作用〕[Effect]

本発明に工って、デユティ比1/100  以下の時分
割駆動において、充分なコントラストが得られる。
With the present invention, sufficient contrast can be obtained in time-division driving with a duty ratio of 1/100 or less.

〔実施列〕[Implementation row]

第1図(a) 、 (b) 、 (C)は、本発明によ
る液晶表示素子の一例を説明する九めの液晶表示素子の
ラビング方向と偏光板の軸との関係を示すモデル図であ
る。同図において、61j上側電極基板のラビング方向
、7は下側電極基板のラビング方向、8は上側偏光板の
吸収軸あるいは偏光軸、9は下側偏光板の吸収軸あるい
は偏光軸、10は液晶分子のねじれ方向および角度、1
1ri上、下側偏光板の吸収軸あるいは偏光軸のなす角
を示し友ものである。
FIGS. 1(a), (b), and (C) are model diagrams showing the relationship between the rubbing direction of the ninth liquid crystal display element and the axis of the polarizing plate, illustrating an example of the liquid crystal display element according to the present invention. . In the figure, 61j is the rubbing direction of the upper electrode substrate, 7 is the rubbing direction of the lower electrode substrate, 8 is the absorption axis or polarization axis of the upper polarizing plate, 9 is the absorption axis or polarization axis of the lower polarizing plate, and 10 is the liquid crystal Molecular twist direction and angle, 1
1ri indicates the angle formed by the absorption axis or polarization axis of the upper and lower polarizing plates.

すなわち、上側電極基板の2ピング方向6と液晶分子配
向とがほぼ一致し、下f11極基板のラビング方向7と
液晶分子配向とがほぼ一致し、そして液晶分子のねじれ
方向および角度10が200度以上の範囲となる工うに
上側電極基板と下側電極基板とが対向配置される。この
場合、この液晶分子のねじれ方向おLび角度10は上、
下電極基板の間に挾持させるネマチック液晶に、液晶分
子のねじれ方向お工び角度10の誘起する施光性物質を
添加し、その混合液晶のらせんのピッチPが液晶層の厚
さdと少なくとも?<3 (1の関係をもつ工うにする
ことにJ:り、液晶分子は200度以上の範囲にねじれ
構造tとることができる。一方、上側偏光板の吸収軸8
と下側閤光板の吸収軸9となす角11は、60度から1
20度までの範囲となるように上a偏光板は上側電極基
板の外面に、下側偏光板は下側電極基板の外面にそれぞ
れ配電されている。なお、偏光板の情は吸収軸の代りに
偏光軸を使用しても工い。
That is, the 2-pin direction 6 of the upper electrode substrate almost matches the liquid crystal molecule orientation, the rubbing direction 7 of the lower f11 electrode board almost matches the liquid crystal molecule orientation, and the twist direction and angle 10 of the liquid crystal molecules are 200 degrees. In order to achieve the above range, the upper electrode substrate and the lower electrode substrate are arranged facing each other. In this case, the twist direction L and angle 10 of this liquid crystal molecule are above,
A photochromic substance that induces a twisting angle of 10 in the twist direction of liquid crystal molecules is added to the nematic liquid crystal sandwiched between the lower electrode substrates, and the helical pitch P of the mixed liquid crystal is at least equal to the thickness d of the liquid crystal layer. ? <3 (In order to have the relationship of
The angle 11 formed between this and the absorption axis 9 of the lower light plate is 60 degrees to 1
The upper a polarizing plate is electrically distributed to the outer surface of the upper electrode substrate, and the lower polarizing plate is electrically distributed to the outer surface of the lower electrode substrate so that the range is up to 20 degrees. Note that the polarizing plate can also be used with the polarizing axis instead of the absorption axis.

第3図は、一対の偏光板の吸収軸のなす角度が90eで
ある′rN形液晶表示素子の鉛直方向の電圧−輝度特性
を示し友ものである。同図においてi4I&が10%に
なる電圧t”Vto s 909kになる電圧t”Ve
・とするとき、時分割駆動特性を表わす量βを β” Vto/ Ve。
FIG. 3 shows the voltage-luminance characteristics in the vertical direction of a 'rN type liquid crystal display element in which the angle between the absorption axes of a pair of polarizing plates is 90e. In the same figure, the voltage t”Vto s at which i4I& becomes 10% and the voltage t”Ve at which 909k
・When , the quantity β representing the time division drive characteristic is β” Vto/Ve.

と定義する。セしてβは1以上の値を示し、1に近づく
程時分割駆動特性が良−ことを表わしている。
It is defined as In this case, β shows a value of 1 or more, and the closer it gets to 1, the better the time-division drive characteristics are.

lf、エステルミクロヘキサン(KCH)系液晶を主成
分とし九混合液晶を使用して、△ndΣα5μ嘴液晶分
子のねじれ角90度と240度の条件で、電圧に対する
セルの容にtCの変化を測定し九ところ、第4図に示す
ような結果が得られt0曲曲線はねじれ90度、曲線す
はねじれ角240度の場合である。
Using a nine-mixed liquid crystal mainly composed of lf, ester microhexane (KCH) liquid crystal, we measured the change in tC in the cell capacity with respect to voltage under conditions of twist angles of 90 degrees and 240 degrees for the △ndΣα5μ beak liquid crystal molecules. However, results as shown in FIG. 4 were obtained, in which the t0 curve has a twist of 90 degrees and the curve has a twist angle of 240 degrees.

第4図エフ明らかな二うに液晶分子のねじれ角が90度
に比べ240度の方が容量Cの急しゅん性が現われ、双
安定性を示した。この工うな急しゅん性は200度以上
で顕著になる。
As is clear from FIG. 4, the capacitance C becomes more abrupt when the twist angle of the liquid crystal molecules is 240 degrees than when it is 90 degrees, indicating bistability. This suddenness becomes noticeable at temperatures above 200 degrees.

更に△n d :15μm、一対の偏光板の吸収軸のな
す角度が90度の条件で、液晶分子のねじれ角と時分割
特性値βを測定しtところ、第5図に示すような結果が
得られ几。
Furthermore, the twist angle of the liquid crystal molecules and the time-division characteristic value β were measured under the conditions that Δnd: 15 μm and the angle between the absorption axes of the pair of polarizing plates was 90 degrees, and the results were as shown in Figure 5. Obtained.

第5図より明らかなように液晶分子のねじれ角が200
度以上でねじれ角90度1ク良い値を示し次。このいず
れの値もデユティ比17100  の実効電比1.10
5を下まわり、デユーティ比1/100駆動でスタテッ
ク駆動量のコントラストが得られる。
As is clear from Figure 5, the twist angle of the liquid crystal molecules is 200
The torsion angle of 90 degrees or more shows a good value. Both values are effective power ratio 1.10 with duty ratio 17100.
5 and a duty ratio of 1/100 driving provides contrast in static driving amount.

ま几更に△ndχ15μm、液晶分子のねじれ角が24
0度の条件で、上偏光板の吸収軸と上側基板のラビング
方向を一致させると一対の偏光板の吸収軸のなす角に対
する選択部の透過率を測定したところ、第6図に示すよ
うな結果が得られ几。
Furthermore, △ndχ15μm, the twist angle of liquid crystal molecules is 24
When the absorption axis of the upper polarizing plate and the rubbing direction of the upper substrate were made to match under the 0 degree condition, the transmittance of the selected part with respect to the angle formed by the absorption axes of the pair of polarizing plates was measured, as shown in Figure 6. I got the results.

第6図より明らかなように一対の偏光板の吸収軸のなす
角が90度付近で選択部の透過率が最も小さくなジ、コ
ントラスト比が良くなる。しかし一対の偏光板の吸収軸
のなす角が60度以下及び120度以上では透過率が3
0チ以上になり充分なコントラスト比が取れない。し九
がって、一対の偏光板の吸収軸のなす角が60度から1
20度までの範囲が好ましい。ま几上偏光板の吸収軸と
上側基板のラビング方向のなす角は0度から50度が最
もコントラストが良い。
As is clear from FIG. 6, when the angle formed by the absorption axes of the pair of polarizing plates is around 90 degrees, the transmittance of the selective portion is the smallest, and the contrast ratio is improved. However, if the angle formed by the absorption axes of a pair of polarizing plates is less than 60 degrees or more than 120 degrees, the transmittance will be 3.
The contrast ratio becomes more than 0 and a sufficient contrast ratio cannot be obtained. Therefore, the angle formed by the absorption axes of a pair of polarizing plates is 60 degrees to 1
A range of up to 20 degrees is preferred. The best contrast is obtained when the angle between the absorption axis of the upper polarizing plate and the rubbing direction of the upper substrate ranges from 0 degrees to 50 degrees.

第7図に本発明の構造の一例を示す。ラビングに二って
配向処理し北上下の電極基板100゜101を対向させ
、上下の′Ii極基板100,101をシール剤にエフ
!J[L、その間隙に正の銹′1異方性をもつ7j E
 CH系ネマチック液晶102を封入し、上下偏光板1
05,104をそれぞれ上下電極基板100,101の
外面に配置させt0更に上偏光板103の吸収軸105
は上電極基板10Gのラビング方向106に一致させて
いる。
FIG. 7 shows an example of the structure of the present invention. The upper and lower north electrode substrates 100° 101 are aligned by rubbing, and the upper and lower 'Ii electrode substrates 100, 101 are used as a sealant. J[L, 7j E with positive ru'1 anisotropy in the gap
Filled with CH-based nematic liquid crystal 102, upper and lower polarizing plates 1
05 and 104 are arranged on the outer surfaces of the upper and lower electrode substrates 100 and 101, respectively.
is made to coincide with the rubbing direction 106 of the upper electrode substrate 10G.

下偏光板104の吸収軸107は、上偏光板105の吸
収軸105と90度なしている。液晶分子のねじれ角は
240度である。
The absorption axis 107 of the lower polarizing plate 104 is at 90 degrees with the absorption axis 105 of the upper polarizing plate 105. The twist angle of liquid crystal molecules is 240 degrees.

g7図(a)(b)(c)にて、上側よジ上偏光板10
5に鉛直方向に入つt光は、上偏光板105に通ると直
線偏光になり、TN液晶層を通過することに工9、だ円
偏光になる。(a)は原理説明図、(b)はOFF状態
の説明図、(C)はON状態の説明図である。液晶の屈
折率異方性△nと液晶層の厚さdの積△ndは、[lL
7μm以下になると、だ日車がやや大きくなり、液晶の
ねじれに追ずいできない几め、だ円の長袖方向が上′電
極基板100の2ピング方向106と約90度−なす方
向になり、下偏光板104の吸収軸107の方向とほぼ
一致する。すなわち電圧印加のない状態では明るくなる
。ところが電圧印加すると液晶分子は立ち、上偏光板1
05を通過し九直編偏光はそのまま下偏光板104の吸
収軸107に吸収される。すなわち電圧印加の状態では
暗くなる。液晶の屈折率異方性△nと液晶層の唯さd’
7)積△ndが12μm以下になると、だ円の長袖方向
が上電極基板100のラビング方向106となす角が小
さくなり、暗くなる。しtかって液晶の屈折率異方性△
nと液晶1の厚さdの積△n(lは、12μmから(1
7μmまでの範囲が好ましい。
g7 In Figures (a), (b), and (c), the upper polarizing plate 10
When the light enters vertically into the upper polarizing plate 105, it becomes linearly polarized light, and when it passes through the TN liquid crystal layer, it becomes elliptically polarized light. (a) is an explanatory diagram of the principle, (b) is an explanatory diagram of the OFF state, and (C) is an explanatory diagram of the ON state. The product Δnd of the refractive index anisotropy Δn of the liquid crystal and the thickness d of the liquid crystal layer is [lL
If it is less than 7 μm, the date wheel becomes a little larger and cannot follow the twisting of the liquid crystal, so the long sleeve direction of the oval is approximately 90 degrees from the second pin direction 106 of the upper electrode substrate 100, and the lower This almost coincides with the direction of the absorption axis 107 of the polarizing plate 104. In other words, it becomes brighter when no voltage is applied. However, when voltage is applied, the liquid crystal molecules stand up and the upper polarizing plate 1
05, the nine straight-polarized light is absorbed as it is by the absorption axis 107 of the lower polarizing plate 104. That is, it becomes dark when voltage is applied. Refractive index anisotropy △n of liquid crystal and thickness d' of liquid crystal layer
7) When the product Δnd becomes 12 μm or less, the angle that the long sleeve direction of the ellipse makes with the rubbing direction 106 of the upper electrode substrate 100 becomes smaller and becomes darker. However, the refractive index anisotropy of liquid crystal △
The product of n and the thickness d of the liquid crystal 1 △n (l is from 12 μm to (1
A range of up to 7 μm is preferred.

〔発明の効果〕〔Effect of the invention〕

以上説明し7t=うに本発明に:れば、時分Xll 嘔
動特性の優れ九液晶表示装置が実現できる。
According to the present invention as described above, a liquid crystal display device with excellent oscillation characteristics can be realized.

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

第11引吐←+〒←は、本角明による液晶表示素子のラ
ビング方向と閤光板の軸との関係を示した説明図、第2
図は従来のTNM液晶表示素子のラビング方向と偏光軸
との関係を示した説明図、第5図は時分割H&特性の定
義に用いられる液晶表示素子の電圧−輝度!身性を示す
説明図、第4図C本発明の実施例の容icと印加電圧の
関係を示す説明図、M5図は本発明の実施例の液晶分子
のねじれ角と時分割駆動特性との関係を示す説明図、第
6因は本発明の実施例の液晶分子のねじれ角と選択部の
透過率の関係を示す説明図、第7図は本発明の実施例の
液晶表示素子の構造を示す説明図である。 以   上 出頓人 セイコーニブノン株式会社 代理人 弁理± 1 上    務 v90v′O印加電圧 第3図 第4図 摩晶分多−ねじ?fj4  (皮) 第5図 411丸ffl/’1jLQK軸tr’jJ角 1度】
第6図 四−一−1 第7図
11th drawing←+〒← is an explanatory diagram showing the relationship between the rubbing direction of a liquid crystal display element and the axis of a light plate by Akira Honkaku,
The figure is an explanatory diagram showing the relationship between the rubbing direction and the polarization axis of a conventional TNM liquid crystal display element, and Fig. 5 is a voltage-luminance! Figure 4C is an explanatory diagram showing the relationship between capacitance IC and applied voltage in the embodiment of the present invention, and Figure M5 is an explanatory diagram showing the relationship between the twist angle of liquid crystal molecules and the time-division drive characteristic in the embodiment of the present invention. The sixth factor is an explanatory diagram showing the relationship between the twist angle of the liquid crystal molecules and the transmittance of the selective part in the embodiment of the present invention. Figure 7 is the diagram showing the structure of the liquid crystal display element in the embodiment of the present invention. FIG. The above person is the representative of Seiko Nibunon Co., Ltd., a patent attorney. fj4 (skin) Fig. 5 411 circleffl/'1jLQK axis tr'jJ angle 1 degree]
Figure 6 4-1-1 Figure 7

Claims (2)

【特許請求の範囲】[Claims] (1)対向して配置する2枚の電極基板間にねじれ配向
したネマチック液晶を挾持してなる液晶セルと前記液晶
セルを挾んで両側に配置された一対の偏光板とを備え、
前記ネマチック液晶はねじれ角が200度以上の範囲を
有し、前記一対の偏光板の吸収軸あるいは偏光軸のなす
角が、60度から120度までの範囲を有し、前記ネマ
チック液晶の屈折率異方性△nと該液晶の厚さdとの積
△n・dが0.2μmから0.7μmまでの範囲内とな
るように設定したことを特徴とする液晶表示素子。
(1) A liquid crystal cell comprising a twisted oriented nematic liquid crystal sandwiched between two electrode substrates disposed facing each other, and a pair of polarizing plates disposed on both sides sandwiching the liquid crystal cell,
The nematic liquid crystal has a twist angle of 200 degrees or more, the angle formed by the absorption axis or polarization axis of the pair of polarizing plates is in the range of 60 degrees to 120 degrees, and the refractive index of the nematic liquid crystal is A liquid crystal display element characterized in that the product Δn·d of the anisotropy Δn and the thickness d of the liquid crystal is set within a range of 0.2 μm to 0.7 μm.
(2)前記ネマチック液晶のねじれ角が220度から2
60度までの範囲を有することを特徴とする特許請求の
範囲第一項の液晶表示素子。
(2) The twist angle of the nematic liquid crystal is from 220 degrees to 2
A liquid crystal display element according to claim 1, characterized in that it has a range of up to 60 degrees.
JP60287410A 1985-12-20 1985-12-20 Liquid crystal display element Pending JPS62247329A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60287410A JPS62247329A (en) 1985-12-20 1985-12-20 Liquid crystal display element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60287410A JPS62247329A (en) 1985-12-20 1985-12-20 Liquid crystal display element

Publications (1)

Publication Number Publication Date
JPS62247329A true JPS62247329A (en) 1987-10-28

Family

ID=17716970

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60287410A Pending JPS62247329A (en) 1985-12-20 1985-12-20 Liquid crystal display element

Country Status (1)

Country Link
JP (1) JPS62247329A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62296121A (en) * 1986-06-17 1987-12-23 Stanley Electric Co Ltd Liquid-crystal display element
JPS636524A (en) * 1986-06-26 1988-01-12 Stanley Electric Co Ltd Liquid crystal display element
JPS6374030A (en) * 1986-09-12 1988-04-04 エフ ホフマン―ラ ロシュ アーゲー Liquid crystal display
DE3918828A1 (en) * 1989-06-09 1990-12-13 Licentia Gmbh Twisted nematic cell type LCD - has greater view angle in larger operating temp. range with less background noise

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6052827A (en) * 1983-09-02 1985-03-26 Hitachi Ltd Liquid crystal display element
JPS6073525A (en) * 1983-09-30 1985-04-25 Hitachi Ltd Liquid crystal display element
JPS60107020A (en) * 1983-07-12 1985-06-12 ビ−ビ−シ− アクチエンゲゼルシヤフト ブラウン ボヴエリ ウント コムパニ− Liquid crystal display

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60107020A (en) * 1983-07-12 1985-06-12 ビ−ビ−シ− アクチエンゲゼルシヤフト ブラウン ボヴエリ ウント コムパニ− Liquid crystal display
JPS6052827A (en) * 1983-09-02 1985-03-26 Hitachi Ltd Liquid crystal display element
JPS6073525A (en) * 1983-09-30 1985-04-25 Hitachi Ltd Liquid crystal display element

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62296121A (en) * 1986-06-17 1987-12-23 Stanley Electric Co Ltd Liquid-crystal display element
JPS636524A (en) * 1986-06-26 1988-01-12 Stanley Electric Co Ltd Liquid crystal display element
JPS6374030A (en) * 1986-09-12 1988-04-04 エフ ホフマン―ラ ロシュ アーゲー Liquid crystal display
DE3918828A1 (en) * 1989-06-09 1990-12-13 Licentia Gmbh Twisted nematic cell type LCD - has greater view angle in larger operating temp. range with less background noise

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