JPH027074B2 - - Google Patents
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- Publication number
- JPH027074B2 JPH027074B2 JP59242875A JP24287584A JPH027074B2 JP H027074 B2 JPH027074 B2 JP H027074B2 JP 59242875 A JP59242875 A JP 59242875A JP 24287584 A JP24287584 A JP 24287584A JP H027074 B2 JPH027074 B2 JP H027074B2
- Authority
- JP
- Japan
- Prior art keywords
- liquid crystal
- pixel
- electrodes
- active matrix
- crystal layer
- 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
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- Liquid Crystal (AREA)
- Liquid Crystal Display Device Control (AREA)
- Devices For Indicating Variable Information By Combining Individual Elements (AREA)
Description
【発明の詳細な説明】
産業上の利用分野
本発明は情報機器ないし映像機器に使用される
高性能の液晶表示装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a high-performance liquid crystal display device used in information equipment or video equipment.
従来例の構成とその問題点
一般にX−Yマトリクス型液晶表示装置では、
X電極とY電極は第1図に示す如く、平行帯状電
極群より成り、これらが液晶層をはさみ互に直交
するように配置され、電極交点部分が1画素に相
当しており、1画素内では、周辺の電界の乱れを
無視すれば、平等電界が印加される様に構成され
ている。しかるに、大量の情報を表示する為の画
素数の多いマトリクス型表示パネルでは、クロス
トークを防止し鮮明な表示を達成するには、各画
素は電気光学特性に於て明確な閾値特性を有して
いなければならず、もつぱら液晶材料の特性向上
に期待がよせられている。Conventional configuration and its problems Generally, in an X-Y matrix type liquid crystal display device,
As shown in Figure 1, the X electrode and the Y electrode consist of a group of parallel band-shaped electrodes, which are arranged to be orthogonal to each other across the liquid crystal layer, and the intersection of the electrodes corresponds to one pixel, and the area within one pixel is In this case, if disturbances in the surrounding electric field are ignored, the structure is such that a uniform electric field is applied. However, in matrix type display panels with a large number of pixels to display a large amount of information, each pixel must have a clear threshold characteristic in its electro-optical characteristics in order to prevent crosstalk and achieve clear display. Therefore, expectations are high for improving the properties of liquid crystal materials.
一方、X−Y電極間に液晶をはさみ込んだ、い
わゆる単純マトリクス型の表示装置では、上に述
べた閾値特性の不十分さ故に映像等の大容量表示
が困難なことから各画素に薄膜トランジスタ(以
下TFTと略す)、MOS−FET、非直線抵抗素子
(バリスタ、ダイオード、MIMなど)等を付加す
るいわゆるアクテイブマトリクスの開発が盛んで
あり、既にTFTやMOS−FETを導入したアクテ
イブマトリクス型液晶テレビが市販されるに到つ
ている。 On the other hand, in so-called simple matrix display devices in which a liquid crystal is sandwiched between X-Y electrodes, it is difficult to display large-capacity images such as images due to the insufficient threshold characteristics mentioned above. The so-called active matrix, which adds TFT (hereinafter abbreviated as TFT), MOS-FET, non-linear resistance elements (varistor, diode, MIM, etc.), etc., is actively being developed, and active matrix LCD TVs that have already incorporated TFT and MOS-FET are actively being developed. has reached the point where it is commercially available.
この様なアクテイブマトリクス型液晶TVでは
表示の目的が映像であるが故に、中間調を忠実に
再生しなければならず、単純マトリクスに於て大
容量の2値表示を実現する時とは、全く逆に、液
晶には、輝度−電圧特性に於て、なだらかなカー
ブを描くものが要求される。 Since the display purpose of such active matrix LCD TVs is video, it is necessary to faithfully reproduce halftones, which is completely different from achieving a large-capacity binary display with a simple matrix. On the contrary, liquid crystals are required to have brightness-voltage characteristics that draw a gentle curve.
現在広く用いられているねじれネマチツク液晶
(以下TN液晶と呼ぶ)は、いずれの用途に於て
も中途半破な特性を示し、走査線数の多い単純マ
トリクスによる2値表示ないし、階調再現性に優
れたアクテイブマトリクス型映像表示のいずれも
不満足な状態であつた。 Twisted nematic liquid crystals (hereinafter referred to as TN liquid crystals), which are currently widely used, exhibit mediocre characteristics in all applications, such as binary display using a simple matrix with a large number of scanning lines, and gradation reproducibility. All of the active matrix type video displays, which were excellent in quality, were unsatisfactory.
発明の目的
本発明は、コントラストに優れた大容量の単純
マトリクスによる2値表示ないし、階調再現性に
優れたアクテイブマトリクス型映像表示を実現す
ることを目的とする。OBJECTS OF THE INVENTION It is an object of the present invention to realize a binary display using a large capacity simple matrix with excellent contrast or an active matrix type video display with excellent gradation reproducibility.
発明の構成
本発明の液晶表示装置は、液晶層をはさむ一対
の電極が、1画素を単位として、少くとも一方が
点状ないし線状の溝を設けることによつて模様状
に形成されてあり、液晶層に強制的に不均一電界
を印加し、従来の如き、平等電界が印加されるよ
うに構成された装置では達成しえなかつた電気光
学特性を実現するところに特徴を有する。Structure of the Invention In the liquid crystal display device of the present invention, a pair of electrodes sandwiching a liquid crystal layer are formed in a pattern by providing dotted or linear grooves on at least one of them for each pixel. , is characterized in that it forcibly applies a non-uniform electric field to the liquid crystal layer and achieves electro-optical characteristics that could not be achieved with conventional devices configured to apply a uniform electric field.
実施例の説明
以下図面に従つて本発明の液晶表示装置の構成
についてのべる。DESCRIPTION OF EMBODIMENTS The structure of a liquid crystal display device of the present invention will be described below with reference to the drawings.
TN液晶セルは電極面に対して液晶分子が若干
のチルト角を有する状態でほぼ平行に配列し、上
下電極間で分子が互に90゜ねじれる様に配向させ
てあり、パネルの外側には、一対の偏光板が偏光
軸が互に平行(ネガ型)ないし垂直(ポジ型)に
なる様に設けられている。偏光板の偏光軸の方向
は、最も近い液晶分子の方向に一致しているか直
交するかいずれかである。 In a TN liquid crystal cell, the liquid crystal molecules are arranged almost parallel to the electrode surface with a slight tilt angle, and the molecules are oriented so that they are twisted by 90 degrees between the upper and lower electrodes. A pair of polarizing plates are provided so that their polarization axes are parallel to each other (negative type) or perpendicular to each other (positive type). The direction of the polarization axis of the polarizing plate is either coincident with or perpendicular to the direction of the nearest liquid crystal molecules.
実際のネガ型TNセルの輝度Bと印加電圧Vの
関係を第2図曲線1で示す。これは第1図に示す
如き電極構成の場合、すなわち1画素に相当する
液晶部分には、実質的に平等電圧が印加される場
合の特性である。第2図の輝度−電圧特性に於
て、輝度が10%変化する電圧を閾値電圧VTとい
い、輝度が90%変化する電圧をVSとすると、閾
値特性γとは、γ=VS/VTで与えられ、単純マ
トリクスで大容量表示を実現するには、γ値がで
きるだけ1に近い特性が要求され、一方、アクテ
イブマトリクス等に於て階調を忠実に再現しよう
とすると、駆動電圧の許す範囲内でできるだけ大
きなγ値を示す液晶が要求される。 The relationship between the brightness B and the applied voltage V of an actual negative-type TN cell is shown by curve 1 in FIG. This is a characteristic when the electrode configuration is as shown in FIG. 1, that is, when substantially equal voltages are applied to the liquid crystal portion corresponding to one pixel. In the brightness-voltage characteristics shown in Figure 2, if the voltage at which the brightness changes by 10% is called the threshold voltage V T and the voltage at which the brightness changes by 90% is called V S , then the threshold characteristic γ is γ = V S /V T , and in order to realize a large capacity display with a simple matrix, the γ value is required to be as close to 1 as possible.On the other hand, when trying to faithfully reproduce gradations with an active matrix, A liquid crystal that exhibits a γ value as large as possible within the voltage range is required.
すなわち前者の目的には曲線2の特性が、後者
の目的には曲線3の特性が望ましい訳である。そ
の為に従来は、上記目的に応じて液晶材料組成を
変える手法が主としてとられていたが、γ値を変
えると必然的に応答速度や、使用温度範囲、閾値
電圧等が変わつてしまい、目的に合つた液晶材料
組成を見出すことははなはだ困難な作業であり、
総合的な特性からみて、γ値には相当な妥協を強
いられるのが実情である。 That is, the characteristics of curve 2 are desirable for the former purpose, and the characteristics of curve 3 are desirable for the latter purpose. To this end, the main method used in the past was to change the composition of the liquid crystal material according to the above objectives, but changing the γ value inevitably changes the response speed, operating temperature range, threshold voltage, etc. Finding a suitable liquid crystal material composition is an extremely difficult task.
In view of the overall characteristics, the reality is that a considerable compromise is forced on the γ value.
本発明は、セルのγ値を変化させるのに、画素
に印加される電界の強度分布も深く係つているこ
とを見出したことに基づく。 The present invention is based on the discovery that the intensity distribution of the electric field applied to the pixel is also deeply involved in changing the γ value of the cell.
すなわち第3図に示す如く、1画素を単位とし
て電極を点状ないし線状の溝を設けることによつ
て模様状に形成し、従来とは異つて、画素に強制
的に不均一電界を印加するように構成すると、一
般に閾値電圧VTの変動を伴うものの、γ値を大
きく変化させうることが見出された。 In other words, as shown in Fig. 3, electrodes are formed in a pattern by providing dotted or linear grooves for each pixel, and, unlike the conventional method, a non-uniform electric field is forcibly applied to each pixel. It has been found that when configured to do so, the γ value can be greatly changed, although the threshold voltage V T is generally fluctuated.
電極の模様は第3図以外に、1画素を単位とし
て描けば、第4図のように種々のものが考えられ
る。いずれにしても通常のマトリクス表示パネル
では、画素の大きさは0.2〜0.5mm程度の正方形な
いし長方形が一般的であり、液晶層をはさむ電極
間ギヤツプは5μm〜10μm程度のものである。 In addition to the pattern shown in FIG. 3, various patterns of electrodes can be considered, as shown in FIG. 4, if each pixel is drawn as a unit. In any case, in a normal matrix display panel, the pixel size is generally square or rectangular with a size of about 0.2 to 0.5 mm, and the gap between the electrodes sandwiching the liquid crystal layer is about 5 μm to 10 μm.
すなわち通常画素の幅は厚みにくらべて数10倍
の、書籍形状であり画素のサイズにくらべて電極
のない部分(図では黒線で示されている)が太す
ぎたり、まばらであつたりすると、画素内部で肉
眼で識別される濃淡が生じて好ましくない。この
様な場合は、たとえば、第3図に示すような4つ
の模様で1画素を構成するように1画素内の模様
を細分化する必要がある。こうすることにより一
画素内の濃淡が見えにくくなる。尚、対向する電
極の一方のみを模様状にしても、両方とも同一な
いし各々異つた模様状に形成した電極を向い合せ
ても液晶層に不均一電界を発生しうるから、目的
に応じた電極の形状を採用すべきである。通常
TN液晶では電極は厚み1000Å前後のスズ入り酸
化インジウムをガラスやプラスチツク基板上に蒸
着ないしスパツタにより成膜した透明電極より成
り、第4図の如き模様は、フオトエツチないしリ
フトオフ法ないしはレーザカツテイング法により
形成できる。いずれにしても、X、Y帯状電極を
横断してしまうと、電極は断線してしまうから、
横切らない範囲内で模様化する必要がある。 In other words, the width of a normal pixel is several tens of times larger than its thickness, so if the part without electrodes (indicated by a black line in the figure) is too thick or sparse compared to the size of the pixel, , undesirable shading occurs inside the pixel that can be discerned with the naked eye. In such a case, it is necessary to subdivide the pattern within one pixel so that one pixel is composed of four patterns as shown in FIG. 3, for example. This makes it difficult to see the shading within one pixel. Note that even if only one of the opposing electrodes is patterned, a non-uniform electric field can be generated in the liquid crystal layer even if both electrodes are formed in the same or different patterns and are faced, so the electrodes should be selected according to the purpose. should be adopted. usually
In TN liquid crystals, the electrodes are transparent electrodes formed by depositing or sputtering tin-containing indium oxide with a thickness of around 1000 Å on a glass or plastic substrate. Can be formed. In any case, if you cross the X and Y strip electrodes, the electrodes will break, so
It is necessary to create a pattern within a range that does not cross.
薄膜トランジスタ等を絵素単位で設けたアクテ
イブマトリクスパネルでは、TFTアレーを構成
した基板側に画素電極を有し、対向電極側は表面
面全面に渡つて均一な共通電極であり、X−Yマ
トリクスは、TFTを設けてある基板側に構成さ
れている。この様な場合は、TFT基板側の各画
素電極を各々第4図の如き模様に構成するか、な
いしは、画素に対応する共通電極側に設けるか、
両者共に設けて、上下電極模様の組合わせ効果を
利用すればよい。 In an active matrix panel in which thin film transistors, etc. are installed in pixel units, the pixel electrode is on the substrate side that constitutes the TFT array, and the counter electrode side is a uniform common electrode over the entire surface, and the X-Y matrix is , is configured on the substrate side where the TFT is provided. In such a case, each pixel electrode on the TFT substrate side should be configured in a pattern as shown in Figure 4, or should be provided on the common electrode side corresponding to the pixels.
Both may be provided to utilize the combined effect of the upper and lower electrode patterns.
従来のような均一電極では、電極面に平行な液
晶層断面では、液晶分子のチルト角、ツイスト角
は一定と見なせたが、不均一電界により駆動され
る本発明のセルでは、ミクロ的に見れば各液晶層
断面に於ても、チルト角、ツイスト角は一定では
ない。γ値に影響する因子は、電極模様、電極溝
幅、長さ及び溝ピツチ、電極間ギヤツプ等のセル
構成パラメータの他、液晶の弾性定数と誘電率、
屈折率異方性等の液晶材料パラメータによつて決
定され、上記セル構成パラメータをどのように設
定すると所定の液晶材料を用いて、γ値を小さく
ないし大きくしうるか、解折的な解を見出すには
到つていない。 With conventional uniform electrodes, the tilt angle and twist angle of liquid crystal molecules can be considered to be constant in the cross section of the liquid crystal layer parallel to the electrode surface, but in the cell of the present invention, which is driven by a nonuniform electric field, As you can see, the tilt angle and twist angle are not constant even in the cross section of each liquid crystal layer. Factors that affect the γ value include cell configuration parameters such as electrode pattern, electrode groove width, length and groove pitch, and gap between electrodes, as well as the elastic constant and dielectric constant of the liquid crystal,
It is determined by liquid crystal material parameters such as refractive index anisotropy, and we will find a analytical solution to how to set the above cell configuration parameters to make the γ value small or large using a given liquid crystal material. has not yet been reached.
発明の効果
本発明においては、所定の液晶材料を用いて、
単に電極を模様化するのみでγ値を操作しうるこ
とが可能であり、単純マトリクス高デユーテイの
大容量表示に有用なだけでなく、映像表示には不
可欠な階調再現を果たしうるセルを構成でき、液
晶を用いた情報機器、映像機器の高性能化に大き
く貢献しうるものである。Effects of the Invention In the present invention, using a predetermined liquid crystal material,
It is possible to manipulate the γ value simply by patterning the electrodes, and the cell is not only useful for simple matrix high-duty, large-capacity display, but also capable of achieving gradation reproduction, which is essential for video display. This technology can greatly contribute to improving the performance of information and video equipment that uses liquid crystals.
第1図は従来のX−Yマトリクス形液晶表示パ
ネルのX、Y電極構成を示す構成図、第2図はネ
ガ型液晶表示セルの輝度−電圧特性を示す特性
図、第3図は本発明の、画素に不均一電界を印加
する為の電極模様の1例を示す図、第4図は本発
明に用いることのできる電極模様の他の例を示す
図である。
1……従来の第1図の電極構成で得られる特性
曲線、2,3……本発明の不均一電界型液晶セル
で得られる特性曲線。
Fig. 1 is a configuration diagram showing the X and Y electrode configuration of a conventional X-Y matrix type liquid crystal display panel, Fig. 2 is a characteristic diagram showing the brightness-voltage characteristics of a negative type liquid crystal display cell, and Fig. 3 is a diagram showing the present invention. FIG. 4 is a diagram showing an example of an electrode pattern for applying a nonuniform electric field to a pixel, and FIG. 4 is a diagram showing another example of an electrode pattern that can be used in the present invention. 1...Characteristic curve obtained with the conventional electrode configuration shown in FIG. 1, 2, 3... Characteristic curve obtained with the non-uniform electric field type liquid crystal cell of the present invention.
Claims (1)
基板間に液晶層がはさまれてなるX−Yマトリク
ス型液晶表示装置に於て、X、Y電極の交点に当
る1画素を単位として、XないしY電極の少くと
も一方が点状ないし線状の溝を設けることによつ
て模様状に形成されてあり、液晶層に不均一電界
を印加するようにしたことを特徴とする液晶表示
装置。 2 アクテイブマトリクスアレーと、これと対向
する電極間に液晶層がはさまれてなるアクテイブ
マトリクス型液晶表示装置に於て、アクテイブマ
トリクスアレー側に設けられた画素電極ないし
は、これと対向する電極の少くとも一方が1画素
を単位として、点状ないし線状の溝を設けること
によつて模様状に形成されてあり、液晶層に不均
一電界を印加するようにしたことを特徴とする液
晶表示装置。[Claims] 1. In an X-Y matrix type liquid crystal display device in which a liquid crystal layer is sandwiched between a pair of substrates having a group of parallel band-shaped electrodes that are orthogonal to each other, For each pixel, at least one of the X or Y electrodes is formed in a pattern by providing dotted or linear grooves to apply a non-uniform electric field to the liquid crystal layer. Characteristic liquid crystal display device. 2. In an active matrix type liquid crystal display device in which a liquid crystal layer is sandwiched between an active matrix array and an electrode facing the active matrix array, a pixel electrode provided on the side of the active matrix array or one of the electrodes facing the active matrix array. A liquid crystal display device characterized in that one of the two is formed in a pattern by providing dotted or linear grooves in units of one pixel, and a non-uniform electric field is applied to the liquid crystal layer. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59242875A JPS61121087A (en) | 1984-11-16 | 1984-11-16 | Liquid crystal display unit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59242875A JPS61121087A (en) | 1984-11-16 | 1984-11-16 | Liquid crystal display unit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61121087A JPS61121087A (en) | 1986-06-09 |
| JPH027074B2 true JPH027074B2 (en) | 1990-02-15 |
Family
ID=17095534
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59242875A Granted JPS61121087A (en) | 1984-11-16 | 1984-11-16 | Liquid crystal display unit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61121087A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH07117666B2 (en) * | 1987-10-09 | 1995-12-18 | 佐藤 進 | Liquid crystal device |
| JPH0812347B2 (en) * | 1989-01-09 | 1996-02-07 | 松下電器産業株式会社 | Liquid crystal element and its driving method |
| JPH087343B2 (en) * | 1989-05-26 | 1996-01-29 | 松下電器産業株式会社 | Liquid crystal element and its driving method |
| KR970000359B1 (en) * | 1991-09-26 | 1997-01-08 | 가부시기가이샤 도오시바 | LCD Display |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5842030A (en) * | 1981-09-07 | 1983-03-11 | Hitachi Ltd | display element |
-
1984
- 1984-11-16 JP JP59242875A patent/JPS61121087A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61121087A (en) | 1986-06-09 |
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|---|---|---|---|
| EXPY | Cancellation because of completion of term |