JPS62244019A - Liquid crystal electro-optical device - Google Patents

Liquid crystal electro-optical device

Info

Publication number
JPS62244019A
JPS62244019A JP8874586A JP8874586A JPS62244019A JP S62244019 A JPS62244019 A JP S62244019A JP 8874586 A JP8874586 A JP 8874586A JP 8874586 A JP8874586 A JP 8874586A JP S62244019 A JPS62244019 A JP S62244019A
Authority
JP
Japan
Prior art keywords
liquid crystal
pieces
optical device
polarizing plates
thickness
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
JP8874586A
Other languages
Japanese (ja)
Inventor
Yuzuru Sato
譲 佐藤
Hiroshi Watabe
渡部 寛
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 JP8874586A priority Critical patent/JPS62244019A/en
Publication of JPS62244019A publication Critical patent/JPS62244019A/en
Pending legal-status Critical Current

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  • Liquid Crystal (AREA)
  • Devices For Indicating Variable Information By Combining Individual Elements (AREA)

Abstract

PURPOSE:To obtain the titled device which is excellent in its storage effect, steepness and orienting property, and has a high contrast ratio, by placing plural pieces of liquid crystal elements between two pieces of polarizing plates. CONSTITUTION:In a liquid crystal electro-optical device which has placed a liquid crystal element between two pieces of roughly orthogonal polarizing plates, two pieces of liquid crystal elements are superposed so that picture elements of the respective liquid crystal elements are superposed each other. As for a response speed and a threshold characteristic, a storage effect, and an orienting property, thickness (d) of a liquid crystal layer 11 is thinned to about 1mum, and the liquid crystal element of this thickness (d) is superposed by (n) pieces and placed between two pieces of polarizing plates 16. In this way, the screen can be brightened.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は液晶電気光学装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a liquid crystal electro-optical device.

〔従来の技術〕[Conventional technology]

従来の液晶電気光学装置においては、2枚の偏光板の間
に唯一枚の液晶素子が挾まれている。
In a conventional liquid crystal electro-optical device, only one liquid crystal element is sandwiched between two polarizing plates.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ツイストネマチック型の液晶素子を使用する場合は特に
問題はない。しかし数μsecで応答し急峻なしきい特
性と記憶効果き持つ強誘電性液晶全使用しようとした。
There are no particular problems when using a twisted nematic type liquid crystal element. However, an attempt was made to use all ferroelectric liquid crystals, which respond in a few microseconds and have steep threshold characteristics and memory effects.

S合、その特性音発現させるためには液晶層の厚さt1
〜2μm程度まで薄くしなければならない。ところが2
枚の直交する偏光板の間に挾んだ時の透過光強度!はs
in” (2πd#n/λ]に比例する念め液晶層の厚
さd’j小さくしていくと1が減少していき、ディスプ
レイとして用い九場合、画面が暗くなる。逆にd′!!
−大きくしていくとしきい特性と記憶効果が悪くなって
コントラスト比が低下し、さらに応答速度は印加電場に
反比例するため、dを大きくすればそれだけ高い電圧を
印加しなければ応答が遅くなる、という問題がある。画
面の明るさについては液晶の複屈折−を大きくすること
で解決できそうであるが、今ni現状(<CL2)より
もさらに大きくすることは容易ではない。
In order to develop the characteristic sound, the thickness t1 of the liquid crystal layer is
It must be made as thin as ~2 μm. However, 2
Intensity of transmitted light when sandwiched between two orthogonal polarizing plates! is s
As the thickness of the liquid crystal layer d'j is proportional to in''(2πd#n/λ), 1 decreases, and when used as a display, the screen becomes dark.On the contrary, d'! !
-As d increases, the threshold characteristics and memory effect worsen, resulting in a decrease in contrast ratio, and the response speed is inversely proportional to the applied electric field, so increasing d will slow down the response unless a higher voltage is applied. There is a problem. It seems that the brightness of the screen can be solved by increasing the birefringence of the liquid crystal, but it is not easy to increase it further than the current situation (<CL2).

また、強fIs電性液晶を配向させることはネマチツり
液晶の場合よりかなり難しく、液晶層が厚くなるほど配
向性が悪くなる。配向性が悪くなると、OFF状態でも
光が透過し、記憶効果も低下する之め、コントラスト比
が低下してしまう。
Furthermore, it is much more difficult to align a strong fIs-conductive liquid crystal than in the case of a nematic liquid crystal, and the thicker the liquid crystal layer, the worse the alignment becomes. If the orientation deteriorates, light will pass through even in the OFF state, and the memory effect will also deteriorate, resulting in a decrease in contrast ratio.

そこで本発明はこのような問題点勿解決して、高速で応
答し液A−の配向性が良く、コントラスト比が高く表示
画面が明るい液晶1気光学装置金提供することにある。
SUMMARY OF THE INVENTION The object of the present invention is to solve these problems and provide a liquid crystal optical device that responds at high speed, has good orientation of liquid A, has a high contrast ratio, and has a bright display screen.

〔問題点?解決するための手段〕〔problem? Means to solve]

まず応答速度としきい特性、記憶効果、配向性に関して
は液晶1′1#の厚さdを1μmaKまで薄くすること
で確保する。そして、この厚さdの液晶素子全n枚(m
≧2)重ねて2枚の偏光板の間に挾む。こうすること(
(よってsin”(2πmdTh/λ)が大さくなって
画面を明るくすることができる。表示装置として使用す
る場合、通常は白色光全便う念め、透過光に巳がつかず
、しかも最も明るくなる条件はレターデーションが0.
25μm程夏で6ることなので、main :[125
μmとなるように使用する液晶材料の+fiに応じてm
(!:dk選べばよい。
First, the response speed, threshold characteristics, memory effect, and orientation are ensured by reducing the thickness d of the liquid crystal 1'1# to 1 μmaK. Then, a total of n liquid crystal elements (m
≧2) Stacked and sandwiched between two polarizing plates. To do this (
(Thus, sin" (2πmdTh/λ) becomes larger and the screen can be made brighter. When used as a display device, it is usually necessary to use white light, so that the transmitted light does not have a shadow and is the brightest. The condition is that the retardation is 0.
Since it is about 25 μm in summer, main: [125
m depending on the +fi of the liquid crystal material used so that it becomes μm.
(!: Just choose dk.

〔実施例〕〔Example〕

第1図に本発明による液晶′亀気元学装置の断面図?示
す。11は液晶層、12は配向″制御膜、15はガラス
!&、i4は走査電極、15は信号電極、16は遍元仮
、17はスペーサー、そして18は一枚の液晶素子を表
わす。第1図はそれぞれの液晶素子の画素が重なり合う
ように2枚の液晶菓子(m=2)t’[ねてbる。
FIG. 1 is a cross-sectional view of a liquid crystal device according to the present invention. show. 11 is a liquid crystal layer, 12 is an alignment control film, 15 is glass!&, i4 is a scanning electrode, 15 is a signal electrode, 16 is an elemental layer, 17 is a spacer, and 18 is a single liquid crystal element. In Figure 1, two liquid crystal sweets (m=2) are laid down so that the pixels of each liquid crystal element overlap.

第1の実月例として、Δn=[L16の液晶材料?使用
し九〇第2図に撞々の液晶層厚におけるコントラスト比
を示す。d ) 1.5μmでは記憶効果が得られずコ
ントラスト比は1となるが5eLk小さくしていけばコ
ントラスト比lユ上昇していった。そこでmdΔnzI
IL25μmになるようにm = 2 、d = (L
 75μmとして液晶電気光学装置全作成し念。m==
1、d=1.5μmの場合と表示時性r比較丁nば、コ
ントラスト比は1.5から27へ改善され、良好な表示
が得られた。第2因によれば、m ” 1 、d ”:
 (L75μmの時のコントラスト比は20であり、そ
の液晶;(子t2枚重ねた時(m=2、d=α75μm
)のコントラスト比と一致していない。それは、ON状
態の透過元強度工ONはsin’(2πmdAn/λ)
に比例するために、2枚重ねることによって工QMが増
加してコントラスト比が増加したのである。
As a first actual example, Δn=[LCD material of L16? Figure 90 shows the contrast ratio for various liquid crystal layer thicknesses. d) At 1.5 μm, no memory effect is obtained and the contrast ratio is 1, but as the thickness is decreased by 5eL, the contrast ratio increases by lU. Therefore, mdΔnzI
m = 2, d = (L
All liquid crystal electro-optical devices were made with a thickness of 75 μm. m==
When comparing the display characteristics with the case where d=1.5 μm, the contrast ratio was improved from 1.5 to 27, and a good display was obtained. According to the second factor, m ” 1 , d ”:
(The contrast ratio when L is 75 μm is 20, and the liquid crystal;
) does not match the contrast ratio. That is, the transmission source strength factor ON in the ON state is sin'(2πmdAn/λ)
Therefore, by stacking two sheets, the QM increases and the contrast ratio increases.

第2の実施例として、Δn=12の液晶材料を使用した
。この場合、液晶層厚が1μm以上ではコントラスト比
は1であった。そこでm=5、d=α5μmとすること
によってコントラスト20の良好な表示か得られ念。
As a second example, a liquid crystal material with Δn=12 was used. In this case, the contrast ratio was 1 when the liquid crystal layer thickness was 1 μm or more. Therefore, by setting m = 5 and d = α5 μm, a good display with a contrast of 20 can be obtained.

第3の実施例としてΔn=[Li2の液晶材料ケ使用し
た。この」場合はd=2.Qμmとしてもコントラスト
比は6が得られたが、m=2、a=1.0μmとするこ
とによってコントラスト比t26まで高くすることがで
きた。
In the third example, a liquid crystal material with Δn=[Li2 was used. In this case, d=2. Although a contrast ratio of 6 was obtained even with Qμm, by setting m=2 and a=1.0μm, the contrast ratio could be increased to t26.

液晶)−へ印加できる電圧はIO耐圧のほぼ1/2まで
という制限があるため、印加電圧?それ以上に高くして
応答を速くすることはできない。
Since the voltage that can be applied to the liquid crystal (liquid crystal) - is limited to approximately 1/2 of the IO breakdown voltage, the applied voltage? It is not possible to increase the response speed any higher than that.

しかし、いずれの実施例においても、dΔn:(L25
となるe、a!−厚dOに対する印加電、IAn−KO
とすればm = 2父は5として各液晶素子の厚さでd
o/2又はdO/3としであるため、各液晶層に印加さ
れる電場は2Ko又は3Eoとなり応答は2倍又は3倍
に速くなっている。
However, in any of the examples, dΔn:(L25
becomes e, a! - applied voltage versus thickness dO, IAn-KO
Then, m = 2 and 5, and the thickness of each liquid crystal element is d.
Since it is set to o/2 or dO/3, the electric field applied to each liquid crystal layer is 2Ko or 3Eo, making the response twice or three times faster.

〔発明の効果〕〔Effect of the invention〕

本発明の構成によれば、従来技術においては一枚の液晶
素子t2枚の41j4元枚に挾んでいたところt2枚以
上に分割して個々の液晶層厚を薄くし之ことにより、記
憶効果、急峻性、配向性にすぐれて高いコントラスト比
が得られ、表示画面が明るくしかも応答の速い液晶電気
光学長ifk作成することができる。本発明は大型ディ
スプレイ、光変調器などに応用することができる。
According to the structure of the present invention, in the conventional technology, one liquid crystal element is sandwiched between two 41J quaternary sheets, but by dividing it into two or more sheets and reducing the thickness of each liquid crystal layer, the memory effect, It is possible to create a liquid crystal electro-optical length ifk with excellent steepness and orientation, a high contrast ratio, a bright display screen, and a fast response. The present invention can be applied to large displays, optical modulators, etc.

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

第1図は本発明による液晶畦気光岸装貢の断面図、第2
図はコントラスト比の液晶層厚依存性?示す図である。 11、  g晶ノ曽−− 12、配向制御膜 1五 ガラス基敬 14、  走査′〜E極 1り、信号電極 1& 偏光板 1Z スペーサー 1a げ晶素子。 以上 ′31 図
FIG. 1 is a cross-sectional view of the liquid crystal ridge light bank according to the present invention, and FIG.
Does the figure show the dependence of contrast ratio on liquid crystal layer thickness? FIG. 11. Crystal No. 12. Orientation control film 15. Glass base 14. Scan' to E pole 1. Signal electrode 1 & polarizing plate 1Z. Spacer 1a. Crystal element. Above’31 Figure

Claims (2)

【特許請求の範囲】[Claims]  (1)2枚のほぼ直交する偏光板の間に液晶素子を挾
んだ液晶電気光学装置において、その2枚の偏光板の間
に複数枚の液晶素子を挾んだことを特徴とする液晶電気
光学装置。
(1) A liquid crystal electro-optical device in which a liquid crystal element is sandwiched between two substantially orthogonal polarizing plates, characterized in that a plurality of liquid crystal elements are sandwiched between the two polarizing plates.
(2)前記複数枚の各液晶素子の画素が重なり合うよう
に前記液晶素子が重ね合わされていることを特徴とする
特許請求の範囲第1項記載の液晶電気光学装置。
(2) The liquid crystal electro-optical device according to claim 1, wherein the liquid crystal elements are stacked so that the pixels of each of the plurality of liquid crystal elements overlap.
JP8874586A 1986-04-17 1986-04-17 Liquid crystal electro-optical device Pending JPS62244019A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8874586A JPS62244019A (en) 1986-04-17 1986-04-17 Liquid crystal electro-optical device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8874586A JPS62244019A (en) 1986-04-17 1986-04-17 Liquid crystal electro-optical device

Publications (1)

Publication Number Publication Date
JPS62244019A true JPS62244019A (en) 1987-10-24

Family

ID=13951450

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8874586A Pending JPS62244019A (en) 1986-04-17 1986-04-17 Liquid crystal electro-optical device

Country Status (1)

Country Link
JP (1) JPS62244019A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0229629A (en) * 1988-07-19 1990-01-31 Ricoh Co Ltd Liquid crystal element
JPH02275416A (en) * 1989-04-17 1990-11-09 Sharp Corp Liquid crystal display device
US5157524A (en) * 1988-09-30 1992-10-20 Commissariat A L'energie Atomique Apparatus and method for displaying levels of greys on a matrix type display screen
US5392142A (en) * 1990-03-23 1995-02-21 Canon Kabushiki Kaisha Display apparatus with chiral smectic and polymer liquid crystal films, each having birefringent first state and not birefringent second state

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0229629A (en) * 1988-07-19 1990-01-31 Ricoh Co Ltd Liquid crystal element
US5157524A (en) * 1988-09-30 1992-10-20 Commissariat A L'energie Atomique Apparatus and method for displaying levels of greys on a matrix type display screen
JPH02275416A (en) * 1989-04-17 1990-11-09 Sharp Corp Liquid crystal display device
US5392142A (en) * 1990-03-23 1995-02-21 Canon Kabushiki Kaisha Display apparatus with chiral smectic and polymer liquid crystal films, each having birefringent first state and not birefringent second state
US5568283A (en) * 1990-03-23 1996-10-22 Canon Kabushiki Kaisha Optical modulation device and display apparatus with three birefringent films each acting as a half waveplate

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