JP2612504B2 - Liquid crystal device - Google Patents
Liquid crystal deviceInfo
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- JP2612504B2 JP2612504B2 JP2090414A JP9041490A JP2612504B2 JP 2612504 B2 JP2612504 B2 JP 2612504B2 JP 2090414 A JP2090414 A JP 2090414A JP 9041490 A JP9041490 A JP 9041490A JP 2612504 B2 JP2612504 B2 JP 2612504B2
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- liquid crystal
- angle
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- substrates
- alignment
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Description
【発明の詳細な説明】 [発明の分野] 本発明は、電界の方向に応じてコントラストを識別す
ることができる強誘電性液晶を用いた液晶装置に関す
る。Description: FIELD OF THE INVENTION The present invention relates to a liquid crystal device using a ferroelectric liquid crystal capable of distinguishing contrast depending on the direction of an electric field.
[従来技術] 双安定性を有する液晶素子の使用がクラーク(Clar
k)及びラガールウォール(Lagerwall)の両者により特
開昭56-107216号公報、米国特許第4,367,924号明細書等
で提案されている。双安定性液晶としては、一般にカイ
ラルスメクチックC相(SmC*)又はH相(SmH*)を有す
る強誘電性液晶が用いられ、これらの状態において、印
加された電界に応答して第1の光学的安定状態と第2の
光学的安定状態とのいずれかをとり、かつ電界が印加さ
れていないときはその状態を維持する性質、即ち双安定
性を有し、また電界の変化に対する応答がすみやかで、
高速かつ記憶型の表示装置等の分野における広い利用が
期待されている。[Prior Art] The use of a bistable liquid crystal device has been
k) and Lagerwall, both of which are proposed in JP-A-56-107216 and U.S. Pat. No. 4,367,924. In general, a ferroelectric liquid crystal having a chiral smectic C phase (SmC * ) or an H phase (SmH * ) is used as the bistable liquid crystal. In these states, the first optical element responds to an applied electric field. One of the optically stable state and the second optically stable state, and has the property of maintaining the state when no electric field is applied, that is, it has bistability, and has a quick response to a change in the electric field. so,
It is expected to be widely used in fields such as high-speed and storage type display devices.
この強誘電性液晶素子で用いている一対の基板の内側
に、それぞれストライプ状電極群を設け、このストライ
プ状電極が互いに直行するように配線したマトリクス表
示装置とした場合では、例えば特開昭59-193426号公
報、同59-193427号公報、同60-156046号公報や同60-156
047号公報などに開示された駆動法を適用することがで
きる。In the case of a matrix display device in which stripe electrode groups are provided inside a pair of substrates used in the ferroelectric liquid crystal element and the stripe electrodes are wired so as to be perpendicular to each other, for example, Japanese Patent Laid-Open No. -193426, 59-193427, 60-156046 and 60-156
The driving method disclosed in, for example, Japanese Patent No. 047 can be applied.
第2図はその駆動波形の一例で、一走査線上の選択期
間内に「黒」消去位相、選択的「白」書込み位相の
2種の期間を設ける方式を図示したものである。の消
去位相では、走査電極に正の電圧を加えることにより該
走査線上の全又は所定画素を第1の安定状態(以下
「黒」消去の状態とよぶ)にする。の期間では逆に走
査電極に負の電圧を印加し、第2の安定状態(以下
「白」の状態とよぶ)に反転させたい画素(選択画素)
に対応した情報電極にのみに選択的に正の電圧を印加
し、それ以外の画素(半選択画素)に対応した情報電極
には負の電圧を印加する。これによって選択画素には閾
値以上、半選択画素には閾値以下の反転電界が生じ、選
択画素には「白」が書込まれ、半選択画素は「黒」の状
態を保持する。このとき印加する消去位相と書き込み位
相の電圧値の絶対値は通常等しい。FIG. 2 shows an example of the driving waveform, and shows a method of providing two types of periods of a “black” erasing phase and a selective “white” writing phase within a selection period on one scanning line. In the erasing phase, a positive voltage is applied to the scanning electrode to bring all or predetermined pixels on the scanning line into a first stable state (hereinafter referred to as a "black" erasing state). On the other hand, during the period, a negative voltage is applied to the scanning electrode to reverse the pixel to a second stable state (hereinafter referred to as a “white” state) (selected pixel).
, A positive voltage is selectively applied only to the information electrodes corresponding to, and a negative voltage is applied to the information electrodes corresponding to the other pixels (half-selected pixels). As a result, an inversion electric field that is equal to or greater than the threshold value for the selected pixel and equal to or less than the threshold value for the half-selected pixel is generated, “white” is written to the selected pixel, and the half-selected pixel maintains the “black” state. At this time, the absolute values of the voltage values of the erase phase and the write phase applied are usually equal.
ところで、強誘電性液晶の配向制御法として最も一般
的に用いられる、比較的プレチルト角の低いポリイミ
ド、ポリビニルアルコール等の高分子膜をラビング処理
する方法では、通常、見かけのチルト角θが真のチルト
角Θに比べて半分程度に小さくなっている双安定2つの
配向状態(スプレイ配向)が重視される。By the way, in a method of rubbing a polymer film such as polyimide or polyvinyl alcohol having a relatively low pretilt angle, which is most commonly used as a method for controlling the orientation of a ferroelectric liquid crystal, the apparent tilt angle θ is usually a true value. Two bistable alignment states (splay alignment) which are about half smaller than the tilt angle Θ are emphasized.
つまり、基板上に比較的プレチルトの低いLP64(東レ
(株)製)などの配向膜を塗布しラビングしたものを、
上下2枚ラビング方向を同じにして間隙を約1.5μmに
保って貼り合わせてセルを構成し、これにCS1014(チッ
ソ(株)製)などの強誘電性液晶を注入し温度を降下さ
せていくと、第3図(a)〜(e)に示す過程をたど
る。すなわち、高温相からSc*相に転移した直後の同図
(a)に示す状態においてはコントラストの小さい配向
状態(C1配向状態)21および22をとり、温度を下げ、あ
る温度領域に達すると同図(b)に示すようにジグザク
状の欠陥23が発生し、その欠陥を境にしてコントラスト
の高い配向状態(C2配向状態)24と25が現われる。更に
温度が下がるとともにC2配向状態が拡がり(同図
(c),(d))、ついには全体がC2配向状態になる
(同図(e))。In other words, an alignment film such as LP64 (manufactured by Toray Industries, Inc.) with a relatively low pretilt is coated on a substrate and rubbed.
The upper and lower two rubbing directions are the same and the gap is maintained at about 1.5 μm to form a cell, and a ferroelectric liquid crystal such as CS1014 (manufactured by Chisso) is injected into the cell to lower the temperature. And the process shown in FIGS. 3 (a) to 3 (e). That is, in the state shown in FIG. 3A immediately after the transition from the high-temperature phase to the Sc * phase, the alignment states (C1 alignment state) 21 and 22 having a low contrast are taken, and the temperature is lowered. As shown in FIG. 2B, zigzag defects 23 are generated, and alignment states (C2 alignment states) 24 and 25 having high contrast appear from the defect. As the temperature further lowers, the C2 orientation state expands (FIGS. (C) and (d)), and finally the whole becomes the C2 orientation state (FIG. (E)).
C1およびC2の2種類の配向状態は、第4図に示すよう
なスメクチック層のシェプロン構造の違いで説明されて
いる。第4図で、31はスメクチック層、32はC1配向の領
域、33はC2配向の領域を表わす。スメクチック液晶は一
般に層構造をもつがSA相からSC相またはSC *相に転移す
ると層間隔が縮むので第4図のように層が上下基板の中
央で折れ曲った構造(シェブロン構造)をとる。折れ曲
る方向は図に示すようにC1とC2の2つ有り得るがよく知
られているようにラビングによって基板界面の液晶分子
は基板に対して角度をなし(プレチルト)、その方向は
ラビング方向に向かって液晶分子が頭をもたげる(先端
が浮いた格好になる)向きである。このプレチルトのた
めにC1配向とC2配向は弾性エネルギー的に等価でなく、
上述のようにある温度で転移が起こる。また機械的な歪
みで転移が起こることもある。第4図の層構造を平面的
にみると、ラビング方向に向ってC1配向からC2配向に移
るときの境界34はジグザクの稲妻状でライトニング欠陥
と呼ばれ、C2からC1に移るときの環境35は幅の広い、ゆ
るやかな曲線状でヘアピン欠陥と呼ばれる。従来は、該
C1及びC2の配向において、コントラストの観点からC2の
配向状態を用いた液晶素子を提供するものであった。The two types of orientation states, C1 and C2, are explained by the difference in the Sheplon structure of the smectic layer as shown in FIG. In FIG. 4, 31 indicates a smectic layer, 32 indicates a C1-oriented region, and 33 indicates a C2-oriented region. Smectic liquid crystal generally has having a layer structure bent broken in the middle of the layer upper and lower substrates as in the fourth diagram Since S C phase or S C * layer spacing when transition to phase shrinks from S A phase structure (chevron structure) Take. There are two bending directions, C1 and C2, as shown in the figure. As is well known, the liquid crystal molecules at the substrate interface form an angle with the substrate by rubbing (pretilt), and the direction is the rubbing direction. The liquid crystal molecules are leaning toward the head (the tip is floating). Because of this pretilt, C1 orientation and C2 orientation are not equivalent in elastic energy,
Transition occurs at certain temperatures as described above. In addition, transition may occur due to mechanical strain. Looking at the layer structure of FIG. 4 in a plan view, the boundary 34 when shifting from the C1 orientation to the C2 orientation in the rubbing direction is called a lightning defect in a zigzag lightning shape, and the environment 35 when shifting from C2 to C1. Is called a hairpin defect with a wide, gentle curve. Conventionally,
An object of the present invention is to provide a liquid crystal element using the alignment state of C2 from the viewpoint of contrast in the alignment of C1 and C2.
この配向状態を示す素子に例えば第2図に示すような
駆動波形によるマルチプレクシング駆動を適用した場合
は、十分な駆動マージンを確保することができるものの
コントラストではまだ充分なものではなく改良の余地が
あった。For example, when multiplexing drive using a drive waveform as shown in FIG. 2 is applied to an element showing this alignment state, a sufficient drive margin can be secured, but the contrast is still not sufficient and there is room for improvement. there were.
[発明が解決しようとしている課題] よって本発明の目的は、この従来技術の問題点に鑑
み、従来より明るくコントラストの高い表示素子を得る
ことである。そこで、ユニフォーム配向を有する液晶素
子に着目し、該素子に対し、さらに十分な駆動マージン
を確保してコントラストおよび透過率の高い表示が行な
える手段を有した液晶装置を提供することを目的とす
る。[Problems to be Solved by the Invention] Accordingly, an object of the present invention is to provide a display element that is brighter and has a higher contrast than in the related art in view of the problems of the related art. In view of the above, an object of the present invention is to provide a liquid crystal device having a unit capable of performing a display with high contrast and transmittance while securing a sufficient driving margin for the liquid crystal element having a uniform orientation. .
[課題を解決するための手段及び作用] そこで本発明は、走査電極群と情報電極群を備えそれ
ぞれ一軸性配向処理が施こされた一対の基板と、その基
板間に配置された強誘電性液晶とを有する液晶素子と、
互いに極性の異なる消去位相と書き込み位相の2つの位
相から形成され、該消去位相の画素に印加される電圧値
の絶対値が該書き込み位相の画素に印加される電圧値の
絶対値よりも大きい走査信号を走査電極群に印加する手
段とを備えた液晶装置において、液晶素子は、強誘電性
液晶のプレチルト角をα、チルト角をΘ、強誘電性液晶
のカイラルスメクチック層の基板法線に対する傾斜角を
δとすれば、強誘電性液晶が、 Θ<α+δ で表わされる配向状態を有し、かつ該配向状態における
強誘電性液晶が少なくとも2つの安定状態を示し、それ
らの光学軸のなす角度の1/2であるθaと該強誘電性液晶
のチルト角Θとが Θ>θa>Θ/2 で表わされる配向状態を有するようにしている。Means and Solution for Solving the Problems Accordingly, the present invention provides a pair of substrates having a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial orientation treatment, and a ferroelectric substance disposed between the substrates. A liquid crystal element having a liquid crystal;
A scan formed from two phases of an erasing phase and a writing phase having different polarities, wherein the absolute value of the voltage value applied to the pixel in the erasing phase is larger than the absolute value of the voltage value applied to the pixel in the writing phase And a means for applying a signal to the scanning electrode group, wherein the liquid crystal element has a pretilt angle α of the ferroelectric liquid crystal, a tilt angle Θ, and a tilt of the chiral smectic layer of the ferroelectric liquid crystal with respect to the substrate normal. Assuming that the angle is δ, the ferroelectric liquid crystal has an alignment state represented by Θ <α + δ, and the ferroelectric liquid crystal in the alignment state shows at least two stable states, and the angle formed by their optical axes. 1/2 theta a and the tilt angle theta of the ferroelectric liquid crystal is is to have an orientation state represented by Θ> θ a> Θ / 2 in.
あるいは液晶素子は、強誘電性液晶のプレチルト角を
α、チルト角をΘ、強誘電性液晶のカイラルスメクチッ
ク層の基板法線に対する傾斜角をδとすれば、強誘電性
液晶が、 Θ<α+δ で表わされる配向状態を有し、かつ該配向状態における
強誘電性液晶が少なくとも2つの安定状態を示し、それ
らの光学軸のなす角を2等分する位置に一方の偏光板の
吸収軸を合わせ、それに垂直に他方の偏光板の吸収軸を
合わせた配置から一方の偏光板だけを時計方向に3°〜
30°回転させたときの第1の安定状態の呈する色と、反
時計方向に同じ角度回転させたときの第2の安定状態の
呈する色が同じである。Alternatively, in the liquid crystal element, if the pretilt angle of the ferroelectric liquid crystal is α, the tilt angle is Θ, and the tilt angle of the chiral smectic layer of the ferroelectric liquid crystal with respect to the substrate normal is δ, the ferroelectric liquid crystal can be expressed as Θ <α + δ And the ferroelectric liquid crystal in the alignment state shows at least two stable states, and aligns the absorption axis of one of the polarizing plates at a position that bisects the angle between their optical axes. From the arrangement in which the absorption axis of the other polarizer is aligned perpendicularly to the other polarizer, only one
The color of the first stable state when rotated by 30 ° is the same as the color of the second stable state when rotated counterclockwise by the same angle.
あるいは液晶素子は、強誘電性液晶のプレチルト角を
α、チルト角をΘ、強誘電性液晶のカイラルスメクチッ
ク層の基板法線に対する傾斜角をδとすれば、強誘電性
液晶が、 Θ<α+δ で表わされる配向状態を有し、かつ該配向状態における
強誘電性液晶がクロスニコル下、消光位の透過率の低い
2つの安定状態と、クロスニコル下、消光位の透過率の
高い1つまたは2つの安定状態の計3または4状態を有
する。この場合、強誘電性液晶がクロスニコル下、消光
位の透過率の低い第1と第2の2つの安定状態と、クロ
スニコル下、消光位の透過率の高い第3と第4の2つの
安定状態の4つの安定状態を示し、それらの光学軸のな
す角を2等分する位置に一方の偏光板の吸収軸を合わ
せ、それに垂直に他方の偏光板の吸収軸を合わせた配置
から一方の偏光板だけを時計方向に3°〜30°回転させ
たときの第1の安定状態の呈する色と、反時計方向に同
じ角度回転させたときの第2の安定状態の呈する色が同
じであり、一方の偏光板だけを時計方向に3°〜30°回
転させたときの第3の安定状態の呈する色と、反時計方
向に同じ角度回転させたときの第4の安定状態の呈する
色が異なるようにしてもよい。Alternatively, in the liquid crystal element, if the pretilt angle of the ferroelectric liquid crystal is α, the tilt angle is Θ, and the tilt angle of the chiral smectic layer of the ferroelectric liquid crystal with respect to the substrate normal is δ, the ferroelectric liquid crystal can be expressed as Θ <α + δ And the ferroelectric liquid crystal in the alignment state has two stable states with low transmittance at the extinction position under crossed Nicols, and one with high transmittance at the extinction position under crossed Nicols or It has a total of three or four states of two stable states. In this case, the first and second stable states where the ferroelectric liquid crystal has low transmittance at the extinction position under crossed Nicols, and the third and fourth stable states having high transmittance at the extinction position under crossed Nicols. The four stable states of the stable state are shown. The absorption axis of one of the polarizing plates is aligned with a position at which the angle between the optical axes is divided into two, and the absorption axis of the other polarizing plate is aligned perpendicularly to the one. The color that the first stable state exhibits when only the polarizing plate is rotated clockwise by 3 ° to 30 ° is the same as the color that the second stable state exhibits when rotated counterclockwise by the same angle. Yes, the color in the third stable state when only one of the polarizers is rotated clockwise by 3 ° to 30 °, and the color in the fourth stable state when rotated by the same angle in the counterclockwise direction May be different.
あるいは液晶素子は、前記一軸性配向処理の方向が同
一方向であり、強誘電性液晶の主たる配向状態が、基板
間の異物によってまたは基板に歪みを加えることによっ
てヘアピン欠陥およびライトニング欠陥に囲まれた他の
配向状態を生じ、かつこの配向状態が、プレチルトによ
り液晶分子が配向膜表面から浮いている方向に沿ってラ
イトニング欠陥およびヘアピン欠陥の順序で生じるこれ
ら欠陥により囲まれたものであり、前記主たる配向状態
において、強誘電性液晶が少なくとも2つの安定状態を
示し、それらの光学軸のなす角度の1/2であるθaと該強
誘電性液晶のチルト角Θとが Θ>θa>Θ/2 で表わされるようにしてもよい。Alternatively, in the liquid crystal element, the direction of the uniaxial alignment treatment is the same direction, and the main alignment state of the ferroelectric liquid crystal is surrounded by hairpin defects and lightning defects by foreign substances between the substrates or by applying strain to the substrates. Another alignment state is generated, and this alignment state is surrounded by these defects that occur in the order of lightening defects and hairpin defects along the direction in which the liquid crystal molecules float from the alignment film surface due to pretilt. in the alignment state, the ferroelectric liquid crystal exhibits at least two stable states, which is half of the angle between the optical axes thereof theta a and ferroelectric liquid crystal tilt angle theta and the Θ> θ a> Θ It may be represented by / 2.
あるいは液晶素子は、前記一軸性配向処理の方向が同
一方向であり、強誘電性液晶の主たる配向状態が、基板
間の異物によってまたは基板に歪みを加えることによっ
てヘアピン欠陥およびライトニング欠陥に囲まれた他の
配向状態を生じ、かつこの配向状態が、プレチルトによ
り液晶分子が配向膜表面から浮いている方向に沿ってラ
イトニング欠陥およびヘアピン欠陥の順序で生じるこれ
ら欠陥により囲まれたものであり、前記主たる配向状態
において、強誘電性液晶が少なくとも2つの安定状態を
示し、それらの光学軸のなす角を2等分する位置に一方
の偏光板の吸収軸を合わせ、それに垂直に他方の偏光板
の吸収軸を合わせた配置から一方の偏光板だけを時計方
向に3°〜30°回転させたときの第1の安定状態の呈す
る色と、反時計方向に同じ角度回転させたときの第2の
安定状態の呈する色が同じであるようにしてもよい。Alternatively, in the liquid crystal element, the direction of the uniaxial alignment treatment is the same direction, and the main alignment state of the ferroelectric liquid crystal is surrounded by hairpin defects and lightning defects by foreign substances between the substrates or by applying strain to the substrates. Another alignment state is generated, and this alignment state is surrounded by these defects that occur in the order of lightening defects and hairpin defects along the direction in which the liquid crystal molecules float from the alignment film surface due to pretilt. In the aligned state, the ferroelectric liquid crystal shows at least two stable states, the absorption axis of one polarizing plate is aligned with the position at which the angle between the optical axes is bisected, and the absorption axis of the other polarizing plate is perpendicular to it. The color of the first stable state when only one polarizer is rotated clockwise by 3 ° to 30 ° from the alignment of the axes, and the color in the counterclockwise direction Flip color exhibited by the second stable state may be the same obtained while angular rotation.
あるいは液晶素子は、前記一軸性配向処理の方向が同
一方向であり、強誘電性液晶の主たる配向状態が、この
基板間の異物によってまたは基板に歪みを加えることに
よってヘアピン欠陥およびライトニング欠陥に囲まれた
他の配向状態を生じ、かつこの配向状態が、プレチルト
により液晶分子が配向膜表面から浮いている方向に沿っ
てライトニング欠陥およびヘアピン欠陥の順序で生じる
これら欠陥により囲まれたものであり、前記主たる配向
状態における強誘電性液晶はクロスニコル下、消光位の
透過率の低い2つの安定状態と、クロスニコル下、消光
位の透過率の高い1つまたは2つの安定状態の計3また
は4状態を有するようにしてもよい。この場合、前記強
誘電性液晶がクロスニコル下、消光位の透過率の低い第
1と第2の2つの安定状態と、クロスニコル下、消光位
の透過率の高い第3と第4の2つの安定状態の4つの安
定状態を示し、それらの光学軸のなす角を2等分する位
置に一方の偏光板の吸収軸を合わせ、それに垂直に他方
の偏光板の吸収軸を合わせた配置から一方の偏光板だけ
を時計方向に3°〜30°回転させたときの第1の安定状
態の呈する色と、反時計方向に同じ角度回転させた時の
第2の安定状態の呈する色が同じであり、一方の偏光板
だけを時計方向に3°〜30°回転させたときの第3の安
定状態の呈する色と、反時計方向に同じ角度回転させた
時の第4の安定状態の呈する色が異なるようにしてもよ
い。Alternatively, in the liquid crystal element, the direction of the uniaxial alignment treatment is the same direction, and the main alignment state of the ferroelectric liquid crystal is surrounded by hairpin defects and lightning defects by foreign substances between the substrates or by applying strain to the substrates. Other alignment state, and this alignment state is surrounded by these defects that occur in the order of lightning defects and hairpin defects along the direction in which the liquid crystal molecules float from the alignment film surface due to pretilt, and The ferroelectric liquid crystal in the main alignment state has a total of three or four states, that is, two stable states under crossed Nicols and low transmittance at the extinction position and one or two stable states under crossed Nicols and high transmittance at the extinction position. May be provided. In this case, the ferroelectric liquid crystal has the first and second stable states with low transmittance at the extinction position under crossed Nicols, and the third and fourth two states with high transmittance at the extinction position under crossed Nicols. Shows the four stable states of the two stable states, with the absorption axis of one of the polarizing plates aligned at a position that bisects the angle between the optical axes, and the absorption axis of the other polarizing plate aligned perpendicular to it. The color of the first stable state when only one polarizer is rotated clockwise by 3 ° to 30 ° is the same as the color of the second stable state when rotated counterclockwise by the same angle. And a color in the third stable state when only one of the polarizing plates is rotated clockwise by 3 ° to 30 °, and a color in the fourth stable state when rotated by the same angle in the counterclockwise direction. The colors may be different.
あるいは液晶素子は、前記一軸性配向処理の方向が同
一方向であり、強誘電性液晶の主たる配向状態が、基板
間の異物によってまたは基板に歪みを加えることによっ
てヘアピン欠陥およびライトニング欠陥に囲まれた他の
配向状態を生じ、この配向状態は、一軸性配向処理方向
に対してライトニング欠陥およびヘアピン欠陥の順序で
生じるこれら欠陥により囲まれたものであり、前記主た
る配向状態における強誘電性液晶少なくとも2つの安定
状態を示し、それらの光学軸のなす角度の1/2であるθa
と該強誘電性液晶のチルト角Θとが Θ>θa>Θ/2 で表わされるようにしてもよい。Alternatively, in the liquid crystal element, the direction of the uniaxial alignment treatment is the same direction, and the main alignment state of the ferroelectric liquid crystal is surrounded by hairpin defects and lightning defects by foreign substances between the substrates or by applying strain to the substrates. Another alignment state is created, which is surrounded by these defects that occur in the order of lightening defects and hairpin defects with respect to the uniaxial alignment processing direction, and at least two ferroelectric liquid crystals in the main alignment state. Θ a which is one-half of the angle between their optical axes
And the tilt angle の of the ferroelectric liquid crystal may be expressed as Θ> θ a > Θ / 2.
あるいは液晶素子は、前記一軸性配向処理の方向が同
一方向であり、強誘電性液晶の主たる配向状態が、この
基板間の異物によってまたは基板に歪みを加えることに
よってヘアピン欠陥およびライトニング欠陥に囲まれた
他の配向状態を生じ、この配向状態は、一軸性配向処理
方向に対してライトニング欠陥およびヘアピン欠陥の順
序で生じるこれら欠陥により囲まれたものであり、前記
主たる配向状態における強誘電性液晶が少なくとも2つ
の安定状態を示し、それらの光学軸のなす角を2等分す
る位置に一方の偏光板の吸収軸を合わせ、それに垂直に
他方の偏光板の吸収軸を合わせた配置から一方の偏光板
だけを時計方向に3°〜30°回転させたときの第1の安
定状態の呈する色と、反時計方向に同じ角度回転させた
ときの第2の安定状態の呈する色が同じであるようにし
てもよい。Alternatively, in the liquid crystal element, the direction of the uniaxial alignment treatment is the same direction, and the main alignment state of the ferroelectric liquid crystal is surrounded by hairpin defects and lightning defects by foreign substances between the substrates or by applying strain to the substrates. This alignment state is surrounded by these defects that occur in the order of lightening defects and hairpin defects with respect to the uniaxial alignment processing direction, and the ferroelectric liquid crystal in the main alignment state is At least two stable states are shown, and the absorption axis of one of the polarizing plates is aligned at a position bisecting the angle formed by the optical axes, and the polarization axis of one of the polarizing plates is adjusted perpendicularly to the absorption axis of the other polarizing plate. The color of the first stable state when only the plate is rotated clockwise by 3 ° to 30 °, and the second stable state when the plate is rotated counterclockwise by the same angle Color exhibited by the may be the same.
あるいは液晶素子は、前記一軸性配向処理の方向が同
一方向であり、強誘電性液晶の主たる配向状態が、この
基板間の異物によってまたは基板に歪みを加えることに
よってヘアピン欠陥およびライトニング欠陥に囲まれた
他の配向状態を生じ、この配向状態は、一軸性配向処理
方向に対してライトニング欠陥およびヘアピン欠陥の順
序で生じるこれら欠陥により囲まれたものであり、前記
主たる配向状態における強誘電性液晶はクロスニコル
下、消光位の透過率の低い2つの安定状態と、クロスニ
コル下、消光位の透過率の高い1つまたは2つの安定状
態の計3または4状態を有するようにしてもよい。この
場合、強誘電性液晶がクロスニコル下、消光位の透過率
の低い第1と第2の2つの安定状態と、クロスニコル
下、消光位の透過率の高い第3と第4の2つの安定状態
の4つの安定状態を示し、それらの光学軸のなす角を2
等分する位置に一方の偏光板の吸収軸を合わせ、それに
垂直に他方の偏光板の吸収軸を合わせた配置から一方の
偏光板だけを時計方向に3°〜30°回転させたときの第
1の安定状態の呈する色と、反時計方向に同じ角度回転
させたときの第2の安定状態の呈する色が同じであり、
一方の偏光板だけを時計方向に3°〜30°回転させたと
きの第3の安定状態の呈する色と、反時計方向に同じ角
度回転させた時の第4の安定状態の呈する色が異なるよ
うにしてもよい。Alternatively, in the liquid crystal element, the direction of the uniaxial alignment treatment is the same direction, and the main alignment state of the ferroelectric liquid crystal is surrounded by hairpin defects and lightning defects by foreign substances between the substrates or by applying strain to the substrates. This alignment state is surrounded by these defects that occur in the order of lightening defects and hairpin defects with respect to the uniaxial alignment processing direction, and the ferroelectric liquid crystal in the main alignment state is There may be a total of three or four states, that is, two stable states with low transmittance at the extinction position under crossed Nicols and one or two stable states with high transmittance at the extinction position under crossed Nicols. In this case, the first and second stable states where the ferroelectric liquid crystal has low transmittance at the extinction position under crossed Nicols, and the third and fourth stable states having high transmittance at the extinction position under crossed Nicols. It shows four stable states, and the angle between their optical axes is 2
When the absorption axis of one of the polarizing plates is aligned with the position where the light is equally divided, and only the one polarizing plate is rotated clockwise by 3 ° to 30 ° from the arrangement in which the absorption axis of the other polarizing plate is aligned perpendicularly thereto, The color presented by the first stable state is the same as the color presented by the second stable state when rotated by the same angle in the counterclockwise direction,
The color of the third stable state when only one of the polarizers is rotated clockwise by 3 ° to 30 ° is different from the color of the fourth stable state when rotated by the same angle in the counterclockwise direction. You may do so.
あるいは液晶素子は、強誘電性液晶が、配向状態がSm
A相を示す高温域からSm*C相を示す温度域に降温する過
程でライトニング欠陥および/またはヘアピン欠陥の発
生を伴う配向変化がなく、かつ該配向状態における強誘
電性液晶が少なくとも2つの安定状態を示し、それらの
光学軸のなす角度の1/2であるθaと該強誘電性液晶のチ
ルト角Θとが Θ>θa>Θ/2 で表わされるようにしてもよい。Alternatively, the liquid crystal element is composed of a ferroelectric liquid crystal and an alignment state of Sm.
In the process of lowering the temperature from the high temperature region showing the A phase to the temperature region showing the Sm * C phase, there is no alignment change accompanied by the occurrence of lightening defects and / or hairpin defects, and at least two stable ferroelectric liquid crystals in the alignment state shows a state, may be a theta a and ferroelectric properties tilt angle of the liquid crystal theta is half the angle between the optical axes thereof are represented by Θ> θ a> Θ / 2 .
あるいは液晶素子は、強誘電性液晶が、配向状態がSm
A相を示す高温域からSm*C相を示す温度域に降温する過
程でライトニング欠陥および/またはヘアピン欠陥の発
生を伴う配向変化がなく、かつ該配向状態における強誘
電性液晶が少なくとも2つの安定状態を示し、それらの
光学軸のなす角を2等分する位置に一方の偏光板の吸収
軸を合わせ、それに垂直に他方の偏光板の吸収軸を合わ
せた配置から一方の偏光板だけを時計方向に3°〜30°
回転させたときの第1の安定状態の呈する色と、反時計
方向に同じ角度回転させたときの第2の安定状態の呈す
る色が同じであるようにしてもよい。Alternatively, the liquid crystal element is composed of a ferroelectric liquid crystal and an alignment state of Sm.
In the process of lowering the temperature from the high temperature region showing the A phase to the temperature region showing the Sm * C phase, there is no alignment change accompanied by the occurrence of lightening defects and / or hairpin defects, and at least two stable ferroelectric liquid crystals in the alignment state In this state, the absorption axis of one of the polarizing plates is set to a position that bisects the angle between the optical axes, and only one of the polarizing plates is clocked from the arrangement in which the absorption axis of the other polarizing plate is aligned perpendicular to it. 3 ° to 30 ° in the direction
The color of the first stable state when rotated and the color of the second stable state when rotated counterclockwise by the same angle may be the same.
あるいは液晶素子は、強誘電性液晶が、配向状態がSm
A相を示す高温域からSm*C相を示す温度域に降温する過
程でライトニング欠陥および/またはヘアピン欠陥の発
生を伴う配向変化がなく、かつ該配向状態における強誘
電性液晶がクロスニコル下、消光位の透過率の低い2つ
の安定状態と、クロスニコル下、消光位の透過率の高い
1つまたは2つの安定状態の計3または4状態を有する
ようにしてもよい。この場合、強誘電性液晶がクロスニ
コル下、消光位の透過率の低い第1と第2の2つの安定
状態と、クロスニコル下、消光位の透過率の高い第3と
第4の2つの安定状態の4つの安定状態を示し、それら
の光学軸のなす角を2等分する位置に一方の偏光板の吸
収軸を合わせ、それに垂直に他方の偏光板の吸収軸を合
わせた配置から一方の偏光板だけを時計方向に3°〜30
°回転させたときの第1の安定状態の呈する色と、反時
計方向に同じ角度回転させたときの第2の安定状態の呈
する色が同じであり、一方の偏光板だけを時計方向に3
°〜30°回転させたときの第3の安定状態の呈する色
と、反時計方向に同じ角度回転させたときの第4の安定
状態の呈する色が異なるようにしてもよい。Alternatively, the liquid crystal element is composed of a ferroelectric liquid crystal and an alignment state of Sm.
In the process of lowering the temperature from the high temperature region showing the A phase to the temperature region showing the Sm * C phase, there is no alignment change accompanied by the occurrence of a lightning defect and / or a hairpin defect, and the ferroelectric liquid crystal in the alignment state is cross-Nicol, There may be a total of three or four states, two stable states with low transmittance in the extinction position and one or two stable states with high transmittance in the extinction position under crossed Nicols. In this case, the first and second stable states where the ferroelectric liquid crystal has low transmittance at the extinction position under crossed Nicols, and the third and fourth stable states having high transmittance at the extinction position under crossed Nicols. The four stable states of the stable state are shown. The absorption axis of one of the polarizing plates is aligned with a position at which the angle between the optical axes is divided into two, and the absorption axis of the other polarizing plate is aligned perpendicularly to the one. 3 ° to 30 ° clockwise
The color of the first stable state when rotated by the same angle as the color of the second stable state when rotated by the same angle in the counterclockwise direction is the same, and only one of the polarizing plates is rotated clockwise by 3 degrees.
The color of the third stable state when rotated by 30 ° to 30 ° may be different from the color of the fourth stable state when rotated by the same angle in the counterclockwise direction.
あるいは液晶素子は、カイラルスメクチック液晶を有
し、カイラルスメクチック液晶のプレチルト角をα、チ
ルト角をΘ、カイラルスメクチック層の基板法線に対す
る傾斜角をδとした時、該カイラルスメクチック液晶
は、 Θ<α+δ で表わされる配向状態を有し、かつ該配向状態における
カイラルスメクチック液晶が少なくとも2つの安定状態
を示し、それらの光学軸のなす角度の1/2であるθaと該
液晶のチルト角Θとが Θ>θa>Θ/2 の関係を有するようにしてもよい。Alternatively, the liquid crystal element has a chiral smectic liquid crystal, and when the pretilt angle of the chiral smectic liquid crystal is α, the tilt angle is Θ, and the inclination angle of the chiral smectic layer with respect to the substrate normal is δ, the chiral smectic liquid crystal has the following formula: The chiral smectic liquid crystal having an alignment state represented by α + δ, and exhibiting at least two stable states in the alignment state, θa which is a half of the angle between their optical axes, and the tilt angle Θ of the liquid crystal May have a relationship of Θ> θ a > Θ / 2.
[発明の態様の詳細な説明] 第5図は、本発明の強誘電性液晶セルの1例を模式的
に描いたものである。[Detailed Description of Embodiments of the Invention] FIG. 5 schematically depicts an example of the ferroelectric liquid crystal cell of the present invention.
11aと11bは、それぞれIn2O3やITO(Indium Tin Oxid
e)等の透明電極12aと12bで被覆された基板(ガラス
板)であり、その上に200〜3000Å厚の絶縁膜13aと13b
(SiO2膜、TiO2膜、Ta2O5膜など)と、ポリイミドで形
成した、例えば、第12図に示す構造単位を有するポリイ
ミド前駆体から得られる50〜1000Å厚の配向制御膜14a
と14bとがそれぞれ積層されている。配向制御膜14aと14
bは配向方向が、平行かつ同一向き(第1図でいえばA
方向)になるようラビング処理(矢印方向)してある。
基板11aと11bとの間には、強誘電性スメクチック液晶15
が配置され、基板11aと11bとの間の距離は、強誘電性ス
メクチック液晶15のらせん配列構造の形成を抑制するの
に十分に小さい距離(例えば0.1〜3μm)に設定さ
れ、強誘電性スメクチック液晶15は双安定性配向状態を
生じている。上述の十分に小さい距離は、基板11aと11b
との間に配置したビーズスペーサ16(シリカビース、ア
ルミナビーズ)によって保持される。17a,17bは偏光板
である。11a and 11b are In 2 O 3 and ITO (Indium Tin Oxid
e) a substrate (glass plate) covered with transparent electrodes 12a and 12b, etc., on which insulating films 13a and 13b each having a thickness of 200 to 3000 mm
(SiO 2 film, TiO 2 film, Ta 2 O 5 film, etc.) and 50-1000 mm thick alignment control film 14a formed from polyimide, for example, obtained from a polyimide precursor having the structural unit shown in FIG.
And 14b are respectively laminated. Alignment control films 14a and 14
b indicates that the orientation directions are parallel and in the same direction (A in FIG. 1).
Rubbing process (arrow direction).
Between the substrates 11a and 11b, a ferroelectric smectic liquid crystal 15 is provided.
Is set, and the distance between the substrates 11a and 11b is set to a distance (for example, 0.1 to 3 μm) that is small enough to suppress the formation of a helical array structure of the ferroelectric smectic liquid crystal 15. The liquid crystal 15 has a bistable alignment state. The sufficiently small distances described above correspond to the substrates 11a and 11b.
And is held by a bead spacer 16 (silica beads, alumina beads) disposed between them. 17a and 17b are polarizing plates.
ところがその後、本発明者等は特定の配向膜と液晶の
組み合わせを用いると 上記のC1→C2転移が起こりにくく、液晶材料によっ
ては全くC2配向状態が生じないこと、および、 C1配向内に従来見出されていた低コントラストの2
つの安定状態のほかに、コントラストの高い別の2つの
安定状態が現われること を新たに発見した。However, after that, the present inventors found that when a specific alignment film and liquid crystal combination were used, the above C1 → C2 transition was unlikely to occur, and no C2 alignment state was generated depending on the liquid crystal material. Low contrast 2 that was released
In addition to one stable state, we newly discovered that two other high-contrast stable states appear.
そこで、表示素子として画面全体をC1配向状態に統一
し、かつC1配向内の高いコントラストの2状態を白黒表
示の2状態として用いれば、従来より品位の高いディス
プレイができると期待される。つまり、本発明者らは、
強誘電性液晶素子を、強誘電性液晶と、この強誘電性液
晶を間に保持して対向するとともに、その対向面にはそ
れぞれ強誘電性液晶に電圧を印加するための電極が形成
され、かつ強誘電性液晶を配向するための相互にほぼ平
行で同一方向の一軸性配向処理が施された一対の基板と
を備え、強誘電性液晶のプレチルト角をα、チルト角
(コーン角の1/2)をΘ、Sm*C層の傾斜角をδとすれ
ば、強誘電性液晶は、Θ<α+δで表わされる配向状態
を有するようにすると、C1配向状態においてさらにシェ
ブロン構造を有する4つの状態が存在することを確認し
た。この4つのC1状態は、従来のC1状態とは異なってお
り、なかでも4つのC1状態のうちの2つの状態は、双安
定状態(ユニフォーム状態)を形成している。このC1配
向のユニフォーム状態は、従来用いていたC2配向におけ
る双安定状態よりもコントラストが高く、したがって、
このユニフォーム状態において、液晶を駆動させること
により、大きなチルト角θを生じ、高コントラストな画
像がディスプレイされ、且つ残像も生じない。Therefore, if the whole screen is unified into the C1 orientation state as a display element and two states of high contrast in the C1 orientation are used as two states of black-and-white display, it is expected that a display with higher quality than before can be obtained. That is, the present inventors
The ferroelectric liquid crystal element is opposed to the ferroelectric liquid crystal while holding the ferroelectric liquid crystal therebetween, and electrodes for applying a voltage to the ferroelectric liquid crystal are formed on the opposing surfaces, respectively. And a pair of substrates which are substantially parallel to each other and have been subjected to uniaxial alignment processing in the same direction for aligning the ferroelectric liquid crystal. The pretilt angle of the ferroelectric liquid crystal is α, and the tilt angle (1 of cone angle) / 2) is Θ, and the inclination angle of the Sm * C layer is δ. If the ferroelectric liquid crystal has an alignment state represented by Θ <α + δ, four ferroelectric liquid crystals having a further chevron structure in the C1 alignment state are obtained. Confirmed that the state exists. The four C1 states are different from the conventional C1 state, and two of the four C1 states form a bistable state (uniform state). This uniform state of the C1 orientation has higher contrast than the conventionally used bistable state in the C2 orientation, and therefore,
By driving the liquid crystal in this uniform state, a large tilt angle θ is generated, a high-contrast image is displayed, and no afterimage is generated.
以下、上記の、について詳しく説明する。の点
についていうと、C1→C2転移の起こりやすさは、第1表
に示すように、基板界面付近の液晶分子が基板と成す角
度(プレチルト角)と層の傾き角と液晶のチルト角に依
存していた。Hereinafter, the above will be described in detail. As shown in Table 1, the likelihood of the C1 → C2 transition is determined by the angle (pretilt angle) formed by the liquid crystal molecules near the substrate interface with the substrate, the tilt angle of the layer, and the tilt angle of the liquid crystal. Was dependent.
第1表は、プレチルト角の異なる3種類の配向膜A〜
Cのセルにチルト角の異なる3種類の液晶a〜cを注入
して配向状態を見た結果である。ただし、Aの配向膜は
LP64(東レ(株)製)、Bの配向膜はSE610(日産化学
(株)製)、Cの配向膜は第12図で示される構造式のポ
リアミド酸を焼成して得られるポリイミドで、プレチル
ト角はそれぞれ2.5°、6°、12°であった。第1表か
ら、プレチルト角が大きくてコーン角が小さい場合にC1
配向が維持されることが分かる。この結果は以下のよう
に考えれば理解できる。 Table 1 shows three types of alignment films A to A having different pretilt angles.
This is a result of injecting three types of liquid crystals a to c having different tilt angles into the cell C and observing the alignment state. However, the alignment film of A is
LP64 (manufactured by Toray Industries, Inc.), the alignment film of B is SE610 (manufactured by Nissan Chemical Industries, Ltd.), and the alignment film of C is a polyimide obtained by firing polyamic acid having the structural formula shown in FIG. The angles were 2.5 °, 6 °, and 12 °, respectively. From Table 1, when the pretilt angle is large and the cone angle is small, C1
It can be seen that the orientation is maintained. This result can be understood by considering the following.
C1配向、C2配向での基板近くのダイレクタはそれぞれ
第6図(a)および(b)のコーン41上にあるから、チ
ルト角Θ、プレチルト角αおよび層傾斜角δの間には C1配向のとき Θ+δ>α (2) C2配向のとき Θ−δ>α (3) の関係が成り立っていなければならない。層傾斜角δは
チルト層Θより少し小さい値を持つので、チルト角Θの
小さい液晶では、Θ−δも小さく、プレチルト角αが大
きい場合には(3)式の関係が満たされなくなり、C2配
向が現われないのである。したがって、本発明でいうC2
を生ぜずC1配向を生じさせるための条件は Θ−δ<α (4) であることが必要となる。チルト角と層傾斜角は液晶の
温度に依存するので、ある温度で(4)式が成り立って
も、更に低温ではその条件が破れてC2配向が現われるこ
とがある。(4)式の条件はその液晶を表示装置として
用いる全温度範囲で成り立っている必要がある。Since the directors near the substrate in the C1 orientation and the C2 orientation are on the cone 41 in FIGS. 6A and 6B, respectively, the tilt angle Θ, the pretilt angle α, and the layer inclination angle δ When Θ + δ> α (2) When C2 orientation, the relationship of Θ−δ> α (3) must be satisfied. Since the layer inclination angle δ has a value slightly smaller than the tilt layer Θ, the liquid crystal having a small tilt angle Θ has a small Θ−δ and a large pretilt angle α does not satisfy the relationship of the expression (3). No orientation appears. Therefore, C2 in the present invention
It is necessary that the condition for generating the C1 orientation without generating is that Θ−δ <α (4). Since the tilt angle and the layer tilt angle depend on the temperature of the liquid crystal, even if the formula (4) is satisfied at a certain temperature, the condition may be violated at a lower temperature and the C2 orientation may appear. The condition of equation (4) needs to be satisfied over the entire temperature range in which the liquid crystal is used as a display device.
本発明において、プレチルト角αは好ましくは6°<
α<30°より好ましくは8°<α<30°さらに好ましく
は10°<α<30°を示し、Θは7°<α<27°を示し、
δは0<δ<25°を示すとよい。In the present invention, the pretilt angle α is preferably 6 ° <
α <30 °, more preferably 8 ° <α <30 °, still more preferably 10 ° <α <30 °, Θ indicates 7 ° <α <27 °,
δ preferably indicates 0 <δ <25 °.
次にの点について説明する。従来の低プレチルト配
向膜では、C1配向においては比較的コントラストの低い
2つの状態しか安定には存在しえなかった。ところが、
第1表に示した配向膜Cのような高プレチルト配向膜で
は、C1配向のなかに4つの状態が存在して、そのうちの
2つは従来と同じ低コントラストの2状態(偏光顕微鏡
の視野下では消光位がなく青く見えるので液晶のダイレ
クトが上下の基板間でねじれている。以下、スプレイ状
態と呼ぶ)で、ほかの2つはきわだってコントラストの
高い、かつ見掛けのチルト角の大きい状態(偏光顕微鏡
下で消光位がある。以下、ユニフォーム状態と呼ぶ)で
ある。新たに見出されたユニフォーム状態のコントラス
トと透過率はC2配向での値よりも高い。The following points will be described. In the conventional low pretilt alignment film, only two states having relatively low contrast can stably exist in the C1 alignment. However,
In a high pretilt alignment film such as the alignment film C shown in Table 1, there are four states in the C1 alignment, and two of them are in the same low contrast two states as in the prior art (under the visual field of a polarizing microscope). The liquid crystal direct is twisted between the upper and lower substrates because it has no extinction position and looks blue, and the other two are in a state where the contrast is high and the apparent tilt angle is large ( There is an extinction position under a polarizing microscope, which is hereinafter referred to as a uniform state). The contrast and transmittance of the newly found uniform state are higher than those in the C2 orientation.
そしてC1のユニフォーム状態はC1のスプレイ状態に較
べクロスニコル下消光位の透過率が低くC1のスプレイ状
態は2つの状態の区別がつかなくなりユニフォーム2状
態とスプレイ1状態の計3状態のみ観測される場合もあ
る。In the uniform state of C1, the transmittance at the extinction position under cross Nicol is lower than that in the spray state of C1, and the spray state of C1 is indistinguishable between the two states, and only a total of three states of the uniform 2 state and the spray 1 state are observed. In some cases.
第2表はいくつかの液晶のスプレイ状態での無電界時
のみかけのチルト角とθa splayユニフォーム状態でのみ
かけのチルト角θa uniform及びチルト角Θを示したもの
である。表中にはθa splay、θa uniformとΘの比も示し
てある。この表からわかるように同じ液晶材料でもみか
けのチルト角はスプレイ状態で小さくユニフォーム状態
で大きい。Θとの比でみてもスプレイ状態ではθa splay
/Θ<0.4、ユニホーム状態では、θa uniform/Θ>0.5
である。ここで本発明ではC1状態における4つの状態の
うちΘ>θa>Θ/2の関係を示す状態をユニフォーム状
態という。Table 2 shows the tilt angle theta a Uniform and tilt angle Θ apparent in the tilt angle and theta a splay uniform states apparent when no electric field in the splay state of some of the liquid crystal. The table also shows the ratio of θ a splay , θ a uniform and 示 し . As can be seen from this table, even with the same liquid crystal material, the apparent tilt angle is small in the splay state and large in the uniform state. Θ a splay in a splay state also look at the ratio of the Θ
/Θ<0.4, in uniform state, θ a uniform /ユ ニ> 0.5
It is. Here, in the present invention, a state showing a relation of Θ> θ a > を / 2 among the four states in the C1 state is referred to as a uniform state.
そこで、本発明は、強誘電性液晶と、この強誘電性液
晶を間に保持して対向するとともにその対向面にはそれ
ぞれ強誘電性液晶に電圧を印加するための電極が形成さ
れかつ強誘電性液晶を配向するための相互にほぼ平行で
同一方向の一軸性配向処理が施された一対の基板とを備
え、強誘電性液晶のプレチルト角をα、チルト角をΘ、
Sm*C層の傾斜角をδとすれば、強誘電性液晶は、 Θ<α+δ で表わされる配向状態を有し、かつ該配向状態における
強誘電性液晶が少なくとも2つの安定状態を示し、それ
らの光学軸のなす角度の1/2であるθaと該強誘電性液晶
のチルト角Θとが Θ>θa>Θ/2 の関係を満たすC1配向におけるユニフォム状態を表示に
利用しようとするものである。 Therefore, the present invention provides a ferroelectric liquid crystal, and an electrode for applying a voltage to the ferroelectric liquid crystal is formed on the opposing surface while holding the ferroelectric liquid crystal therebetween, and the ferroelectric liquid crystal is formed. A pair of substrates which are substantially parallel to each other and have been subjected to a uniaxial alignment treatment in the same direction for aligning the ferroelectric liquid crystal, wherein the pretilt angle of the ferroelectric liquid crystal is α, the tilt angle is Θ,
Assuming that the inclination angle of the Sm * C layer is δ, the ferroelectric liquid crystal has an alignment state represented by Θ <α + δ, and the ferroelectric liquid crystal in the alignment state shows at least two stable states. trying to use to display the Yunifomu state in the C1 orientation satisfying the tilt angle theta of a half of the angle between the optical axis theta a and ferroelectric liquid crystals Θ> θ a> Θ / 2 in relation Things.
また、本発明でいうC1状態は、セル内のスペーサー等
の異物又はセルに歪みを加えることによってヘアピン欠
陥およびライトニング欠陥にかこまれた他の配向状態を
生じ、プレチルトにより液晶分子が配向膜表面から浮い
ている方向に沿って(即ち液晶分子の配向膜表面近傍の
部分から同液晶分子がプレチルトにより配向膜表面から
浮いている部分に向かう方向に沿って)ライトニング欠
陥、ヘアピン欠陥の順序で生じるこれら欠陥により囲ま
れた他の配向状態が生じる状態、または、セル内のスペ
ーサー等の異物又はセルに歪みを加えることによってヘ
アピン欠陥およびライトニング欠陥にかこまれた他の配
向状態を生じ、ラビング方向に沿ってライトニング欠
陥、ヘアピン欠陥の順序で生じるこれら欠陥で囲まれた
他の配向状態が生じる状態または、スメクチックA(Sm
A)等の高温からカイラルスメチックC(Sm*C)に降温
する過程でライトニング欠陥および/またはヘアピン欠
陥の発生を伴う配向変化がない状態があるということが
いえる。Further, the C1 state referred to in the present invention causes another alignment state surrounded by hairpin defects and lightning defects by applying a strain to a foreign substance such as a spacer in the cell or the cell, and the liquid crystal molecules from the alignment film surface due to pretilt. These lightning defects and hairpin defects are generated in the order of lightening defects and hairpin defects along the floating direction (that is, along the direction from the portion near the alignment film surface of the liquid crystal molecules to the portion where the liquid crystal molecules float from the alignment film surface due to pretilt). A state in which another orientation state surrounded by defects occurs, or another orientation state surrounded by hairpin defects and lightening defects by applying a strain to a foreign substance or a cell such as a spacer in a cell, and the rubbing direction is caused. Other orientation states surrounded by these defects occur in the order of lightning defects, hairpin defects State or, smectic A (Sm
It can be said that there is a state in which there is no orientation change accompanying the occurrence of lightening defects and / or hairpin defects in the process of lowering the temperature from high temperature such as A) to chiral smectic C (Sm * C).
本発明のC1配向におけるスプレイ状態とユニフォーム
状態との違いは前述のみかけのチルト角が違うことの他
にコントラストの違いがある。スプレイ配向は上記のよ
うに、暗状態においてもクロスニコル下で完全な消光位
が得られず、偏光板をクロスニコルから数度捩った位置
に配置するほうがより暗くなる。これに対しユニフォー
ム配向は、クロスニコル下でほぼ完全な消光位がありこ
あために高いコントラスト比を示す。この違いは次のよ
うな測定を行えばいっそうはっきりする。The difference between the splay state and the uniform state in the C1 orientation of the present invention is a difference in contrast in addition to the difference in apparent tilt angle described above. As described above, in the splay orientation, a complete extinction position cannot be obtained under crossed nicols even in a dark state, and it becomes darker when the polarizing plate is arranged at a position twisted several degrees from the crossed nicols. On the other hand, the uniform orientation shows a high contrast ratio because there is almost perfect extinction position under crossed Nicols. This difference becomes even more pronounced when the following measurements are taken.
まずクロスニコル下でアップ・ダウンの2状態のコン
トラストがなくなる位置すなわち2状態の光学軸のなす
角を2等分する方向(スメクチック層方向)に一方の偏
光板の吸収軸を合わせ、これに垂直に他方の偏光板の吸
収軸を合わせる。この位置から検光子(観測者側の偏光
板)だけを時計方向に3°〜30°の適当な角度回転させ
るとアップ・ダウン2状態の透過光状態に差が生じコン
トラストがつく。多くの場合、アップの状態が色濃く見
え、ダウンの状態は色が淡くなる。逆に検光子を反時計
方向に同じ角度回転させると逆の色づきがみられる。す
なわちアップの状態は色淡くなり、ダウン状態は色濃く
なる。First, the absorption axis of one of the polarizing plates is aligned with the position where the contrast between the two states of up and down disappears under crossed Nicols, that is, the direction in which the angle between the optical axes of the two states is bisected (the smectic layer direction). To the absorption axis of the other polarizing plate. When only the analyzer (observer-side polarizing plate) is rotated clockwise at an appropriate angle of 3 ° to 30 ° from this position, a difference occurs in the transmitted light state between the up and down two states, and contrast is obtained. In many cases, the up state looks dark, and the down state becomes pale. Conversely, when the analyzer is rotated counterclockwise by the same angle, the reverse coloring is observed. That is, the up state becomes lighter and the down state becomes darker.
そこでこの検光子回転に対する色づきの様子に着目す
ると、1.0μmないし2.0μmのギャップをもつセルにあ
っては (1) スプレイ配向のアップ・ダウン2状態について
は時計方向に回転したときのップの色は、かっ色ないし
赤紫色であるのに対し反時計方向に回転したときのダウ
ンの色は青色ないし藍色を呈していてこの2つの色は異
なる。一方 (2) ユニフォーム配向のアップ・ダウン2状態につ
いては上記2つの色はともにかっ色ないし赤紫色で同じ
である。この違いは後述のように上下基板間でダイレク
タが捩れているか否かにもとづくものと考ええらるがい
ずれにしてもこの測定からスプレイ配向とユニフォーム
配向を質的に区別することができる。Therefore, focusing on the state of coloring with respect to the rotation of the analyzer, if the cell has a gap of 1.0 μm to 2.0 μm, (1) the up / down state of the splay alignment, and The color is brown or magenta, while the color of the down when rotated in a counterclockwise direction is blue or indigo, and the two colors are different. On the other hand, in the (2) uniform up-down 2 state, the above two colors are either brown or magenta, which are the same. This difference can be considered to be based on whether or not the director is twisted between the upper and lower substrates, as described later. In any case, the spray orientation and the uniform orientation can be qualitatively distinguished from this measurement.
また本発明におけるC1配向の4つの状態は電界をかけ
ると互いに遷移する。弱い正負のパルス電界を印加する
とスプレイ2状態間の遷移が起こり、強い正負のパルス
電界を印加するとユニフォーム2状態間の遷移が起こ
る。ユニフォーム2状態を用いると従来より明るくコン
トラストの高い表示素子が実現できる。In the present invention, the four states of the C1 orientation transition with each other when an electric field is applied. When a weak positive / negative pulse electric field is applied, a transition between the spray 2 states occurs, and when a strong positive / negative pulse electric field is applied, a transition between the uniform 2 states occurs. When the uniform 2 state is used, a brighter and higher-contrast display element can be realized.
ところで、液晶の選択のし方によっては、該ユニフォ
ーム状態の生じやすさに差がある。第1表の配向膜Cを
用いていくつかの液晶でユニフォーム状態の有無を調べ
た結果が第3表である。傾斜角の小さい液晶はユニフォ
ーム状態を取りやすいことが分かる。この原因は必ずし
も明らかではないが、次のようなことが推察される。By the way, there is a difference in the easiness of the uniform state depending on how the liquid crystal is selected. Table 3 shows the results obtained by examining the presence or absence of a uniform state in some liquid crystals using the alignment film C shown in Table 1. It can be seen that the liquid crystal having a small tilt angle easily takes a uniform state. Although the cause is not always clear, the following is presumed.
ユニフォーム状態においては、その光学的性質からみ
てダイレクタが上下基板間でねじれていないと考えられ
る。第7(A)図はC1配向の各状態における基板間の各
位置でのダイレクタの配置を示す模式図である。図中51
〜54は各状態においてダイレクタをコーンの底面に投影
し、これを底面方向から見た様子を示しており、51およ
び52がスプレイ状態、53および54がユニフォム状態と考
えられるダイレクタの配置である。同図から分かるとお
り、ユニフォームの2状態53と54においては、上下いず
れかの基板界面の液晶分子の位置がスプレイ状態の位置
と入れ替わっている。第7(B)図はC2配向を示してお
り界面のスイッチグはなく内部のスイッチングで2状態
がある。第8図は界面分子位置の異なる2つの領域の境
界付近のダイレクタの様子を示したものである。界面分
子の位置は同図に示すようにコーンの頂点60を通って一
方から他方へ移ると考えられるので、チルト角の小さい
ほうが移りやすい。このためチルト角の小さい液晶でユ
ニフォーム状態が実現されるのである。 In the uniform state, it is considered from the optical properties that the director is not twisted between the upper and lower substrates. FIG. 7A is a schematic diagram showing the arrangement of directors at each position between substrates in each state of C1 orientation. In the figure 51
Reference numerals 54 show projections of the director on the bottom surface of the cone in each state, as viewed from the bottom surface direction. Reference numerals 51 and 52 denote splay states, and reference numerals 53 and 54 denote director arrangements considered to be in a uniform state. As can be seen from the figure, in the two states 53 and 54 of the uniform, the position of the liquid crystal molecule at the upper or lower substrate interface is replaced with the position in the spray state. FIG. 7 (B) shows the C2 orientation, in which there is no switching at the interface and there are two states by internal switching. FIG. 8 shows a director near the boundary between two regions having different interface molecular positions. Since the position of the interface molecule is considered to move from one side to the other through the vertex 60 of the cone as shown in the figure, the smaller the tilt angle is, the easier it is to move. For this reason, a uniform state is realized with a liquid crystal having a small tilt angle.
界面の分子が一方の位置から他方の位置へ電界によっ
て移る際に受けるトルクの方向は、分子がコーン上のど
の位置にあるかによって異なる。すなわち、第8図のコ
ーン端61および62よりもプレチルトの高い位置にあれば
コーンの頂点60を通る方向にトルクを受け、逆にコーン
端61および62よりも低い位置にあれば分子は基板に押し
付けられる方向にトルクを受ける。したがって、前者の
位置にあるほうがスイッチングが起こりやすい。プレチ
ルトがコーン端61および62よりも高い位置に来るための
条件は簡単な幾何学的考察により、 sinα>sinδcosθ (5) となり、プレチルト角α、層傾斜角δ、チルト角Θが小
さいときはこの条件は近似的に、 α>δ (6) となる。層傾斜角δはチルト角θに近い値を持つので第
3表に示した実験結果が得られたと解釈される。The direction of the torque that the molecules at the interface undergo when moving from one position to the other by an electric field depends on where the molecules are on the cone. That is, if the pretilt is higher than the cone ends 61 and 62 in FIG. 8, torque is applied in the direction passing through the vertex 60 of the cone, and if the pretilt is lower than the cone ends 61 and 62, the molecules are transferred to the substrate. Receives torque in the direction in which it is pressed. Therefore, switching is more likely to occur in the former position. The condition for the pretilt to be higher than the cone ends 61 and 62 is sinα> sinδcosθ (5) based on simple geometrical considerations. When the pretilt angle α, the layer inclination angle δ, and the tilt angle Θ are small, The condition is approximately α> δ (6). Since the layer inclination angle δ has a value close to the tilt angle θ, it can be interpreted that the experimental results shown in Table 3 were obtained.
よって、C1配向におけるユニフォーム状態をより安定
に形成させるには、さらにδ>αの関係を満たすことが
効果的である。Therefore, in order to more stably form the uniform state in the C1 orientation, it is effective to further satisfy the relationship of δ> α.
又、ユニフォーム状態を安定に形成させるために上下
基板のラビング方向を0〜20°の範囲でずらしたクロス
ラビングも可能である。Further, in order to stably form a uniform state, cross rubbing in which the rubbing directions of the upper and lower substrates are shifted within a range of 0 to 20 ° is also possible.
このようにC1配向におけるユニフォーム2状態を用い
ると従来より明るくコントラストの高い表示素子が実現
できる。As described above, when the uniform 2 state in the C1 orientation is used, a brighter and higher-contrast display element can be realized.
そして本発明は、該C1配向におけるユニフォーム状態
を示す液晶素子に対し好適に駆動させる方法として、走
査電極に印加される走査信号を互いに極性の異なる消去
位相と書き込み位相の2つの位相から形成し、該消去位
相の画素における電圧値の絶対値が該書き込み位相の画
素における電圧値の絶対値よりも大きい走査信号を印加
する手段を適用させるものである。And, the present invention, as a method of suitably driving the liquid crystal element showing a uniform state in the C1 orientation, forming a scanning signal applied to the scanning electrode from two phases of an erasing phase and a writing phase having different polarities, A means for applying a scanning signal in which the absolute value of the voltage value in the pixel in the erase phase is larger than the absolute value of the voltage value in the pixel in the write phase is applied.
それにより、例えば上述のユニフォーム配向が実現さ
れている素子に第2図に示すマルチ・プレクシング駆動
を適用する場合に比べ駆動マージンに関する問題が数段
改善されたより良好な画像が表示できる液晶素子を得る
ことが可能となる。Thereby, for example, a liquid crystal element capable of displaying a better image in which the problem relating to the drive margin is improved by several steps as compared with the case where the multiplex driving shown in FIG. 2 is applied to the element in which the above-described uniform orientation is realized is obtained. It becomes possible.
以下に、本発明の走査信号印加手段の具体例を説明す
る。Hereinafter, a specific example of the scanning signal applying unit of the present invention will be described.
第1図(a)は本発明における駆動波形例を示し、第
1図(b)はその駆動波形を用いて第9図で示した画素
パターンを表示する際のタイミングチャートである。FIG. 1A shows an example of a driving waveform in the present invention, and FIG. 1B is a timing chart when the pixel pattern shown in FIG. 9 is displayed using the driving waveform.
第1図(a)において、SSは走査選択信号波形、SNS
は走査非選択信号波形、IWは白書込み信号波形、Iaは黒
書込み信号波形を表わしている。In FIG. 1A, S S is a scanning selection signal waveform, S NS
The scan non-selection signal waveform, I W is white write signal waveform, I a represents the black write signal waveform.
また、この例では、 V1:V2:V3=3:2:1 t1:t2=2:1 としている。ここで、V1:V2:V3=3:3:1とすると、第
2図の従来例と一致する。In this example, V 1 : V 2 : V 3 = 3: 2: 1 t 1 : t 2 = 2: 1. Here, assuming that V 1 : V 2 : V 3 = 3: 3: 1, this matches the conventional example of FIG.
本発明者等の実験によれば、従来例の駆動波形で駆動
マージンがない原因は半選択時(IB−SS)において、消
去パルス後の半選択パルスによって消去が阻害され、そ
の結果クロストークが発生していることによることが調
べられている。従ってユニフォーム配向においては、書
込みに対してより強い消去過程が必要とされることが明
らかになり、上述のように消去位相の電圧値の絶対値が
書込み位相の電圧値の絶対値よりも大きくなるようにし
ているのである。According to experiments of the present inventors, the cause no drive margin in the driving waveform of the conventional example during half-selected (I B -S S), erase inhibited by half-select pulse after the erase pulse, as a result the cross It has been investigated that a talk is occurring. Therefore, in the uniform orientation, it becomes clear that a stronger erasing process is required for writing, and as described above, the absolute value of the voltage value of the erasing phase is larger than the absolute value of the voltage value of the writing phase. That's how it works.
また、単に消去過程を強く行うのであれば、電圧値を
書込み位相と等しくして、消去位相のパルス幅t1を書込
み位相のパルス幅t2に対して長くすることによっても可
能であるが、t1を長くすることは1ライン選択時間を長
く、フレーム周波数の低下を招くことになり実用上に好
ましくない。Moreover, if simply performed strongly erasing process, to equal the voltage value and the write phase, but it is also possible by lengthening the pulse width t 1 of the erase phase to the pulse width t 2 of the write phase, lengthening the t 1 is longer one line selection time, undesirable practical results in deteriorating the frame frequency.
なお、以上の実験におけるチルト角Θ、層の傾き角
δ、プレチルト角α、みかけのチルト角θaは以下のよ
うにして測定した。Incidentally, the tilt angle Θ in the above experiments, the inclination angle of the layer [delta], the pretilt angle alpha, the tilt angle theta a apparent was measured as follows.
チルト角Θの測定 10V〜30VのDCをFLC素子の上下基板間に印加しなが
ら、直交クロスニコル下、その間に配置されたFLC素子
を偏光板と水平に回転させ第1の消光位(透過率が最も
低くなる位置)をさがし、次に上記と逆極性のDCを印加
しながら第2の消光位をさがす。そして、第1の消光位
から第2の消光位までの角度の1/2をΘとした。Measurement of tilt angle し な が ら While applying DC of 10 V to 30 V between the upper and lower substrates of the FLC element, rotate the FLC element disposed between them under the crossed Nicols horizontally with the polarizing plate and rotate the first extinction position (transmittance) Is lowest), and then the second extinction position is searched for while applying DC of the opposite polarity to that described above. Then, 1/2 of the angle from the first extinction position to the second extinction position was defined as Θ.
みかけのチルト角θaの測定 液晶の閾値の単発パルスを印加した後、無電界下、直
交クロスニコル下その間に配置されたFLC素子を偏光板
と水平に回転させ第1の消光位をさがし、次に上記の単
発パルスと逆極性のパルスを印加した後、無電界下、第
2の消光位をさがす。そして、第1の消光位から、第2
の消光位までの角度の1/2をθaとした。After the application of the tilt angle θ measurement threshold single pulse of the liquid crystal of a apparent, under no electric field, the FLC elements arranged in orthogonal crossed Nicols under therebetween looking for first extinction position by rotating horizontally and a polarizing plate, Next, after applying a pulse having a polarity opposite to that of the above-mentioned single pulse, a second extinction position is searched for under no electric field. Then, from the first extinction position, the second
1/2 of the angle of up to extinction position was θ a.
層の傾き角δの測定 X線解析装置RAD-IIB(45kV,30mA)を用いてX線解析
法でδを測定した。Measurement of Tilt Angle δ of Layer δ was measured by an X-ray analysis method using an X-ray analyzer RAD-IIB (45 kV, 30 mA).
プレチルト角αの測定 Jpn.J.Appl.Phys.vol.19(1980)No.10 Short Notes
2013に記されている方法(クリスタルローテーション
法)に従って求めた。Measurement of pretilt angle α Jpn.J.Appl.Phys.vol.19 (1980) No.10 Short Notes
Determined according to the method described in 2013 (crystal rotation method).
つまり、平行かつ反対方向にラビングした基板をはり
合わせてセル厚20μmのセルを作成し0℃〜60℃の範囲
でSmA相を有する液晶(A)を封入し測定を行った。That is, a substrate having a cell thickness of 20 μm was prepared by bonding substrates rubbed in parallel and in opposite directions, and a liquid crystal (A) having an SmA phase was sealed in a temperature range of 0 ° C. to 60 ° C. for measurement.
液晶セルを上下基板に垂直かつ配向処理軸を含む面で
回転させながら回転軸と45°角度をなす偏光面をもつヘ
リウム・ネオンレーザー光を回転軸に垂直な方向から照
射し、その反対側で入射偏光面と平行な透過軸をもつ偏
光板を通してフォトダイオードで透過光強度を測定し
た。そして、干渉によってできた透過光強度の双曲線群
の中心となる線と液晶セルに垂直な線とがなす角度をφ
xとして下式に代入しプレチルト角α0を求めた。While rotating the liquid crystal cell in a plane perpendicular to the upper and lower substrates and including the alignment axis, a helium-neon laser beam having a polarization plane that forms an angle of 45 ° with the rotation axis is irradiated from the direction perpendicular to the rotation axis. The transmitted light intensity was measured by a photodiode through a polarizing plate having a transmission axis parallel to the incident polarization plane. Then, the angle between the line that is the center of the group of hyperbolas of the transmitted light intensity generated by the interference and the line that is perpendicular to the liquid crystal cell is φ
to determine the pre-tilt angle α 0 is substituted into the following equation as x.
[実施例] 以下、本発明の実施例を説明する。 [Example] Hereinafter, an example of the present invention will be described.
実施例1 透明電極の付いたガラス基板上の酸化タンタルの薄膜
をスパッタ法で形成し、その上に日立化成(株)製のポ
リアミド酸LQ1802の1%NMP溶液をスピンナで塗布し270
℃で1時間焼成した。次に、この基板をラビングし、同
じ処理をしたもう1枚の基板とラビング方向が平行かつ
同方向になるように1.5μmのギャップを保って貼り合
わせセルを作成した。該セルのプレチルト角はクリスタ
ルローテーション法により14°である。該セルにフェニ
ルピリミジンを主成分とする混合液晶で、チルト角は室
温で12°、層傾斜角は室温で10°の強誘電性液晶を注入
した。相転移温度は以下のとおりであった。Example 1 A thin film of tantalum oxide on a glass substrate provided with a transparent electrode was formed by a sputtering method, and a 1% NMP solution of a polyamic acid LQ1802 manufactured by Hitachi Chemical Co., Ltd. was applied on the thin film by a spinner, and then 270.
Calcination was carried out at ℃ for 1 hour. Next, this substrate was rubbed, and a bonded cell was prepared while maintaining a 1.5 μm gap so that the rubbing direction was parallel and the same direction as another substrate subjected to the same treatment. The pretilt angle of the cell is 14 ° by the crystal rotation method. A ferroelectric liquid crystal having a tilt angle of 12 ° at room temperature and a layer tilt angle of 10 ° at room temperature was injected into the cell with a mixed liquid crystal containing phenylpyrimidine as a main component. The phase transition temperatures were as follows.
なお、このセルにおけるパネルの表示面積は、114×2
28mmである。 The display area of the panel in this cell is 114 × 2
28 mm.
以下に、該ユニフォーム状態での表示特性を評価した
結果を示す。The results of evaluating the display characteristics in the uniform state are shown below.
上述の液晶セルを一対の90°クロスニコル偏光子の間
に挟み込んでから、50μsecの30Vパルスを印加してから
90°クロスニコルを消光位(最暗状態)にセットし、こ
の時の透過率をホトマルチプレターにより測定し、続い
て50μsecの−30Vパルスを印加し、この時の透過率(明
状態)の同様の方法で測定したところ、暗状態時の透過
率は0.5%で明状態時の透過率は10%であり、従ってコ
ントラスト比は50:1であった。コントラストのよい素子
となっている。After sandwiching the above-mentioned liquid crystal cell between a pair of 90 ° crossed Nicol polarizers, and then applying a 30 V pulse of 50 μsec,
The 90 ° crossed Nicols is set to the extinction position (darkest state), the transmittance at this time is measured by a photomultiplier, and a −30 V pulse of 50 μsec is applied, and the transmittance (bright state) at this time is measured. When measured in the same manner, the transmittance in the dark state was 0.5% and the transmittance in the bright state was 10%, and thus the contrast ratio was 50: 1. The device has good contrast.
次に上述の強誘電性液晶セルに第1図に示す駆動波形
電圧を以下の条件の下で印加することによって、マルチ
・プレクシング駆動を行った。Next, the multiplexing drive was performed by applying the drive waveform voltage shown in FIG. 1 to the above ferroelectric liquid crystal cell under the following conditions.
V1:V2:V3=3:2:1 t1:t2=2:1 VOP=|V1+V3|=25V その際、室温でパルス幅t2が80〜180μsecの範囲で良
好な画像を表示することができた。V 1 : V 2 : V 3 = 3: 2: 1 t 1 : t 2 = 2: 1 V OP = | V 1 + V 3 | = 25 V At that time, when the pulse width t 2 is in the range of 80 to 180 μsec at room temperature. A good image could be displayed.
即ち、画像表示可能なパルス幅の範囲をtaからtb(tb
>ta)として によって定義されるMを駆動マージンとすると、このと
きの駆動マージンMは0.38であった。That, t the range of the image can be displayed pulse width from t a b (t b
> As t a) Is the drive margin, the drive margin M at this time was 0.38.
これは、V1:V2:V3=3:3:1に設定して画像を形成す
る場合に比べ、より表示画面全体にわたって安定で正常
な表示を得ることができる。This makes it possible to obtain a stable and normal display over the entire display screen as compared with the case where an image is formed by setting V 1 : V 2 : V 3 = 3: 3: 1.
実施例2 第10図(a)に示した駆動波形を用いて第10図(b)
に示したタイミングに従って駆動し、t1:t2=3:2に設
定した他は実施例1と全く同様の方法で画像を形成した
ところ、良好な表示が得られ、M=0.33であった。ま
た、この駆動波形では実施例1に比較して画像のフリッ
カが著しく軽減された。Example 2 FIG. 10B using the driving waveform shown in FIG.
When the image was formed in the same manner as in Example 1 except that the driving was performed according to the timing shown in FIG. 4 and t 1 : t 2 = 3: 2, good display was obtained and M = 0.33. . Further, with this driving waveform, flicker of an image was significantly reduced as compared with the first embodiment.
実施例3 第11図にに示した駆動波形を用いた以外は、実施例2
と全く同様の方法で画像を形成したところ、良好な表示
が得られ、M=0.30あった。また、この駆動波形では、
実施例2に比較してフレーム周波数が約1.7倍増加し
た。Example 3 Example 2 was repeated except that the driving waveform shown in FIG. 11 was used.
When an image was formed in exactly the same manner as in Example 1, good display was obtained, and M = 0.30. In this drive waveform,
The frame frequency increased about 1.7 times as compared with the second embodiment.
[発明の効果] 以上説明したように本発明によれば、液晶素子の全体
にわたって液晶が均一にC1配向状態になるように制御す
るとともに、走査電極に印加される走査信号を互いに極
性の異なる消去位相と書き込み位相の2つの位相から形
成し、消去位相の電圧値の絶対値が該書き込み位相の電
圧値の絶対値よりも大きくなるようにしたため、駆動マ
ージンが十分に大きくなり、コントラストが高く、透過
率の高い画像の表示が可能になる。[Effect of the Invention] As described above, according to the present invention, the liquid crystal element is controlled so as to be uniformly in the C1 alignment state throughout the liquid crystal element, and the scanning signals applied to the scanning electrodes are erased with different polarities. It is formed from two phases, a phase and a writing phase, and the absolute value of the voltage value of the erasing phase is set to be larger than the absolute value of the voltage value of the writing phase. Therefore, the driving margin becomes sufficiently large, and the contrast is high. An image with high transmittance can be displayed.
第1図(a)および(b)は本発明で用いうるマルチ・
プレクシング駆動の駆動電圧の波形図、 第2図は従来例に係る駆動波形図、 第3図(a)〜(e)は強誘電性液晶の冷却過程を示す
説明図、 第4図はC1配向とC2配向の層構造を示す説明図、 第5図は、本発明の強誘電性液晶セルの1例を示す模式
図、 第6図(a)および(b)は基板界面付近のスメクチッ
クC相のコーンとダイレクタを示す模式図、 第7(A)図は、C1配向の各状態における基板間の各位
置でのダイレクタの配置を示す模式図、 第7(B)図は、C2配向の各状態における基板間の各位
置でのダイレクタの配置を示す模式図、 第8図は、界面分子位置の異なる2つの領域の境界付近
のダイレクタの様子を示す模式図、 第9図は本発明の一実施例に係る表示例を示す平面図、 第10図(a)および(b)ならびに第11図は本発明で用
いうる別の好ましい駆動波形の波形図、そして 第12図は配向膜に用いられるポリアミド酸の構造式図で
ある。 SS:走査選択信号波形、SNS:走査非選択信号波形、
IW:白書込み信号波形、IB:黒書込み信号波形、t1:消
去位相のパルス幅、t2:書込位相のパルス幅、21,22:C1
配向状態、24,25:C2配向状態、31:スメクチック層、32:
C1配向の領域、33:C2配向の領域、Θ:コーン角、α:
プレチルト角、δ:層傾斜角。FIGS. 1 (a) and 1 (b) show a multi-unit which can be used in the present invention.
FIG. 2 is a driving waveform diagram of a conventional example, FIG. 3 (a) to (e) are explanatory diagrams showing a cooling process of a ferroelectric liquid crystal, and FIG. 4 is a C1 orientation. FIG. 5 is a schematic view showing an example of a ferroelectric liquid crystal cell of the present invention. FIGS. 6 (a) and (b) are smectic C phases near a substrate interface. FIG. 7 (A) is a schematic diagram showing the arrangement of directors at each position between substrates in each state of C1 orientation, and FIG. 7 (B) is a schematic diagram showing the arrangement of directors in C2 orientation. FIG. 8 is a schematic diagram showing the arrangement of directors at each position between substrates in a state, FIG. 8 is a schematic diagram showing a director near a boundary between two regions having different interfacial molecular positions, and FIG. FIGS. 10 (a) and (b) and FIG. 11 are plan views showing display examples according to the embodiment. FIG. 12 is a structural diagram of a polyamic acid used for an alignment film. S S : Scan selection signal waveform, S NS : Scan non-selection signal waveform,
I W: white write signal waveform, I B: black write signal waveforms, t 1: the pulse width of the erasing phase, t 2: writing phase of the pulse width, 21, 22: C1
Orientation state, 24, 25: C2 orientation state, 31: smectic layer, 32:
C1 oriented area, 33: C2 oriented area, Δ: cone angle, α:
Pretilt angle, δ: layer inclination angle.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 朝岡 正信 東京都大田区下丸子3丁目30番2号 キ ヤノン株式会社内 (72)発明者 内海 俊治 東京都大田区下丸子3丁目30番2号 キ ヤノン株式会社内 (56)参考文献 特開 平3−243920(JP,A) 特開 昭61−267739(JP,A) 特開 平2−273724(JP,A) ──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Masanobu Asaoka 3- 30-2 Shimomaruko, Ota-ku, Tokyo Inside Canon Inc. (72) Inventor Shunji 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon (56) References JP-A-3-243920 (JP, A) JP-A-61-267739 (JP, A) JP-A-2-273724 (JP, A)
Claims (31)
軸性配向処理が施された一対の基板と、その基板間に配
置された強誘電性液晶とを有し、強誘電性液晶のプレチ
ルト角をα、チルト角をΘ、強誘電性液晶のカイラルス
メクチック層の基板法線に対する傾斜角をδとすれば、
強誘電性液晶は、 Θ<α+δ で表わされる配向状態を有し、かつ該配向状態における
強誘電性液晶が少なくとも2つの安定状態を示し、それ
らの光学軸のなす角度の1/2であるθaと該強誘電性液晶
のチルト角Θとが Θ>θa>Θ/2 で表わされる配向状態を有する液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。1. A pretilt of a ferroelectric liquid crystal, comprising a pair of substrates having a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment treatment, and a ferroelectric liquid crystal disposed between the substrates. If the angle is α, the tilt angle is Θ, and the tilt angle of the chiral smectic layer of the ferroelectric liquid crystal with respect to the substrate normal is δ,
The ferroelectric liquid crystal has an alignment state represented by Θ <α + δ, and the ferroelectric liquid crystal in the alignment state shows at least two stable states, and is θ which is 1/2 of the angle formed by their optical axes. a and a tilt angle の of the ferroelectric liquid crystal are formed from a liquid crystal element having an alignment state represented by Θ> θ a > Θ / 2, and two phases having an erasing phase and a writing phase having mutually different polarities, A liquid crystal comprising: means for applying a scanning signal to the scanning electrode group, the scanning signal having an absolute value of a voltage value applied to the pixel in the erasing phase greater than an absolute value of the voltage value applied to the pixel in the writing phase. apparatus.
軸性配向処理が施された一対の基板と、その基板間に配
置された強誘電性液晶とを有し、強誘電性液晶のプレチ
ルト角をα、チルト角をΘ、強誘電性液晶のカイラルス
メクチック層の基板法線に対する傾斜角をδとすれば、
強誘電性液晶は、 Θ<α+δ で表わされる配向状態を有し、かつ該配向状態における
強誘電性液晶が少なくとも2つの安定状態を示し、それ
らの光学軸のなす角を2等分する位置に一方の偏光板の
吸収軸を合わせ、それに垂直に他方の偏光板の吸収軸を
合わせた配置から一方の偏光板だけを時計方向に3°〜
30°回転させたときの第1の安定状態の呈する色と、反
時計方向に同じ角度回転させたときの第2の安定状態の
呈する色が同じである液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。2. A pretilt of a ferroelectric liquid crystal, comprising a pair of substrates provided with a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment treatment, and a ferroelectric liquid crystal disposed between the substrates. If the angle is α, the tilt angle is Θ, and the tilt angle of the chiral smectic layer of the ferroelectric liquid crystal with respect to the substrate normal is δ,
The ferroelectric liquid crystal has an alignment state represented by Θ <α + δ, and the ferroelectric liquid crystal in the alignment state shows at least two stable states, and is located at a position where the angle between the optical axes is bisected. From the arrangement where the absorption axis of one polarizing plate is aligned and the absorption axis of the other polarizing plate is aligned perpendicular to it, only one polarizing plate is turned clockwise by 3 ° or more.
A liquid crystal element having the same color in the first stable state when rotated by 30 ° and the same color in the second stable state when rotated counterclockwise by the same angle; and erasures having different polarities from each other A scan signal formed from two phases, a write phase and a write phase, in which the absolute value of the voltage value applied to the pixel in the erase phase is larger than the absolute value of the voltage value applied to the pixel in the write phase A liquid crystal device comprising: means for applying a voltage to a liquid crystal device.
軸性配向処理が施された一対の基板と、その基板間に配
置された強誘電性液晶とを有し、強誘電性液晶のプレチ
ルト角をα、チルト角をΘ、強誘電性液晶のカイラルス
メクチック層の基板法線に対する傾斜角をδとすれば、
強誘電性液晶は、 Θ<α+δ で表わされる配向状態を有し、かつ該配向状態における
強誘電性液晶がクロスニコル下、消光位の透過率の低い
2つの安定状態と、クロスニコル下、消光位の透過率の
高い1つまたは2つの安定状態の計3または4状態を有
する液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。3. A pretilt of a ferroelectric liquid crystal, comprising a pair of substrates provided with a scanning electrode group and an information electrode group, each of which is subjected to a uniaxial alignment treatment, and a ferroelectric liquid crystal disposed between the substrates. If the angle is α, the tilt angle is Θ, and the tilt angle of the chiral smectic layer of the ferroelectric liquid crystal with respect to the substrate normal is δ,
The ferroelectric liquid crystal has an alignment state represented by Θ <α + δ, and the ferroelectric liquid crystal in the alignment state has two stable states under crossed Nicols and low transmittance in an extinction position, and under crossed Nicols and quenched. Liquid crystal element having a total of three or four stable states of one or two stable states having high transmissivity, and two phases of an erasing phase and a writing phase having different polarities from each other, and applied to a pixel having the erasing phase. A liquid crystal device comprising: means for applying a scanning signal to the scanning electrode group in which the absolute value of the applied voltage value is larger than the absolute value of the voltage value applied to the pixel of the writing phase.
位の透過率の低い第1と第2の2つの安定状態と、クロ
スニコル下、消光位の透過率の高い第3と第4の2つの
安定状態の4つの安定状態を示し、それらの光学軸のな
す角を2等分する位置に一方の偏光板の吸収軸を合わ
せ、それに垂直に他方の偏光板の吸収軸を合わせた配置
から一方の偏光板だけを時計方向に3°〜30°回転させ
たときの第1の安定状態の呈する色と、反時計方向に同
じ角度回転させたときの第2の安定状態の呈する色が同
じであり、一方の偏光板だけを時計方向に3°〜30°回
転させたときの第3の安定状態の呈する色と、反時計方
向に同じ角度回転させたときの第4の安定状態の呈する
色が異なることを特徴とする請求項3記載の液晶装置。4. The first and second stable states in which the ferroelectric liquid crystal has low transmittance at the extinction position under crossed Nicols, and the third and fourth stable states have high transmittance at the extinction position under crossed Nicols. The four stable states of the above two are shown, and the absorption axis of one polarizing plate is aligned with the position where the angle between the optical axes is divided into two equal parts, and the absorption axis of the other polarizing plate is aligned perpendicularly thereto. The color in the first stable state when only one of the polarizers is rotated clockwise by 3 ° to 30 ° from the arrangement, and the color in the second stable state when rotated by the same angle in the counterclockwise direction Are the same, and the color of the third stable state when only one of the polarizing plates is rotated clockwise by 3 ° to 30 °, and the fourth stable state when rotated by the same angle in the counterclockwise direction 4. The liquid crystal device according to claim 3, wherein the color of the liquid crystal is different.
軸性配向処理が施された一対の基板であって該一軸性配
向処理を同一方向とした一対の基板と、その基板間に配
置された強誘電性液晶とを有し、強誘電性液晶の主たる
配向状態は、この基板間の異物によってまたは基板に歪
みを加えることによってヘアピン欠陥およびライトニン
グ欠陥に囲まれた他の配向状態を生じ、かつこの他の配
向状態は、プレチルトにより液晶分子が配向膜表面から
浮いている方向に沿ってライトニング欠陥およびヘアピ
ン欠陥の順序で生じるこれら欠陥により囲まれたもので
あり、前記主たる配向状態において、強誘電性液晶が少
なくとも2つの安定状態を示し、それらの光学軸のなす
角度の1/2であるθaと該強誘電性液晶のチルト角Θとが Θ>θa>Θ/2 で表わされる液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。5. A pair of substrates provided with a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment process, wherein the pair of substrates have the uniaxial alignment process in the same direction, and are disposed between the substrates. Having a ferroelectric liquid crystal, the main alignment state of the ferroelectric liquid crystal is caused by foreign substances between the substrates or by applying a strain to the substrate, causing other alignment states surrounded by hairpin defects and lightning defects, In the other alignment state, the liquid crystal molecules are surrounded by these defects generated in the order of the lightning defect and the hairpin defect along the direction in which the liquid crystal molecules float from the alignment film surface due to the pretilt. ferroelectric liquid crystal exhibits at least two stable states, the table in their one-half of the angle between the optical axis theta a and ferroelectric liquid crystal tilt angle theta and the Θ> θ a> Θ / 2 A liquid crystal element, and an absolute value of a voltage value applied to a pixel having the erase phase and a voltage value applied to the pixel having the write phase, which is formed from two phases of an erase phase and a write phase having different polarities from each other. A liquid crystal device comprising: means for applying a scanning signal larger than the absolute value of the scanning electrode group to the scanning electrode group.
軸性配向処理が施された一対の基板であって該一軸性配
向処理を同一方向とした一対の基板と、その基板間に配
置された強誘電性液晶とを有し、強誘電性液晶の主たる
配向状態は、この基板間の異物によってまたは基板に歪
みを加えることによってヘアピン欠陥およびライトニン
グ欠陥に囲まれた他の配向状態を生じ、かつこの他の配
向状態は、プレチルトにより液晶分子が配向膜表面から
浮いている方向に沿ってライトニング欠陥およびヘアピ
ン欠陥の順序で生じるこれら欠陥により囲まれたもので
あり、前記主たる配向状態において、強誘電性液晶が少
なくとも2つの安定状態を示し、それらの光学軸のなす
角を2等分する位置に一方の偏光板の吸収軸を合わせ、
それに垂直に他方の偏光板の吸収軸を合わせた配置から
一方の偏光板だけを時計方向に3°〜30°回転させたと
きの第1の安定状態の呈する色と、反時計方向に同じ角
度回転させたときの第2の安定状態の呈する色が同じで
ある液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。6. A pair of substrates provided with a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment process, wherein the pair of substrates have the uniaxial alignment process in the same direction, and are disposed between the substrates. Having a ferroelectric liquid crystal, the main alignment state of the ferroelectric liquid crystal is caused by foreign substances between the substrates or by applying a strain to the substrate, causing other alignment states surrounded by hairpin defects and lightning defects, In the other alignment state, the liquid crystal molecules are surrounded by these defects generated in the order of the lightning defect and the hairpin defect along the direction in which the liquid crystal molecules float from the alignment film surface due to the pretilt. The dielectric liquid crystal shows at least two stable states, and aligns the absorption axis of one of the polarizers at a position that bisects the angle between their optical axes;
The same angle in the counterclockwise direction as the color in the first stable state when only one of the polarizing plates is rotated clockwise by 3 ° to 30 ° from the arrangement in which the absorption axis of the other polarizing plate is aligned perpendicularly thereto. A liquid crystal element having the same color in the second stable state when rotated, and a voltage value formed from two phases of an erasing phase and a writing phase having mutually different polarities and applied to a pixel having the erasing phase A means for applying a scanning signal whose absolute value is larger than the absolute value of the voltage value applied to the pixel in the writing phase to the scanning electrode group.
軸性配向処理が施された一対の基板であって該一軸性配
向処理を同一方向とした一対の基板と、その基板間に配
置された強誘電性液晶とを有し、強誘電性液晶の主たる
配向状態は、この基板間の異物によってまたは基板に歪
みを加えることによってヘアピン欠陥およびライトニン
グ欠陥に囲まれた他の配向状態を生じ、かつこの他の配
向状態は、プレチルトにより液晶分子が配向膜表面から
浮いている方向に沿ってライトニング欠陥およびヘアピ
ン欠陥の順序で生じるこれら欠陥により囲まれたもので
あり、前記主たる配向状態における強誘電性液晶はクロ
スニコル下、消光位の透過率の低い2つの安定状態と、
クロスニコル下、消光位の透過率の高い1つまたは2つ
の安定状態の計3または4状態を有する液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。7. A pair of substrates provided with a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment process, wherein the pair of substrates have the uniaxial alignment process in the same direction, and are disposed between the substrates. Having a ferroelectric liquid crystal, the main alignment state of the ferroelectric liquid crystal is caused by foreign substances between the substrates or by applying a strain to the substrate, causing other alignment states surrounded by hairpin defects and lightning defects, The other alignment state is surrounded by these defects that occur in the order of lightning defects and hairpin defects along the direction in which the liquid crystal molecules float from the alignment film surface due to pretilt. Liquid crystal has two stable states under crossed Nicols with low extinction transmittance,
A liquid crystal element having a total of 3 or 4 states of one or two stable states with high transmittance in the extinction position under crossed Nicols, and two phases of an erasing phase and a writing phase having polarities different from each other. A liquid crystal device comprising: means for applying a scan signal to a scan electrode group, the scan signal having an absolute value of a voltage value applied to a pixel of a phase greater than an absolute value of a voltage value applied to a pixel of the write phase.
位の透過率の低い第1と第2の2つの安定状態と、クロ
スニコル下、消光位の透過率の高い第3と第4の2つの
安定状態の4つの安定状態を示し、それらの光学軸のな
す角を2等分する位置に一方の偏光板の吸収軸を合わ
せ、それに垂直に他方の偏光板の吸収軸を合わせた配置
から一方の偏光板だけを時計方向に3°〜30°回転させ
たときの第1の安定状態の呈する色と、反時計方向に同
じ角度回転させた時の第2の安定状態の呈する色が同じ
であり、一方の偏光板だけを時計方向に3°〜30°回転
させたときの第3の安定状態の呈する色と、反時計方向
に同じ角度回転させた時の第4の安定状態の呈する色が
異なることを特徴とする請求項7記載の液晶装置。8. The first and second stable states in which the ferroelectric liquid crystal has a low transmittance at an extinction position under crossed Nicols, and the third and fourth stable states have a high transmittance at an extinction position under crossed Nicols. The four stable states of the above two are shown, and the absorption axis of one polarizing plate is aligned with the position where the angle between the optical axes is divided into two equal parts, and the absorption axis of the other polarizing plate is aligned perpendicularly thereto. The color in the first stable state when only one polarizer is rotated clockwise by 3 ° to 30 °, and the color in the second stable state when rotated counterclockwise by the same angle. Are the same, the color of the third stable state when only one of the polarizing plates is rotated clockwise by 3 ° to 30 °, and the fourth stable state when the same polarizer is rotated counterclockwise by the same angle 8. The liquid crystal device according to claim 7, wherein the colors of the liquid crystal display are different.
軸性配向処理が施された一対の基板であって該一軸性配
向処理を同一方向とした一対の基板と、その基板間に配
置された強誘電性液晶とを有し、強誘電性液晶の主たる
配向状態は、この基板間の異物によってまたは基板に歪
みを加えることによってヘアピン欠陥およびライトニン
グ欠陥に囲まれた他の配向状態を生じ、この他の配向状
態は、一軸性配向処理方向に沿ってライトニング欠陥お
よびヘアピン欠陥の順序で生じるこれら欠陥により囲ま
れたものであり、前記主たる配向状態における強誘電性
液晶は少なくとも2つの安定状態を示し、それらの光学
軸のなす角度の1/2であるθaと該強誘電性液晶のチルト
角Θとが Θ>θa>Θ/2 で表される液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。9. A pair of substrates provided with a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment process, wherein the pair of substrates have the uniaxial alignment process in the same direction, and are disposed between the substrates. Having a ferroelectric liquid crystal, the main alignment state of the ferroelectric liquid crystal is caused by foreign substances between the substrates or by applying a strain to the substrate, causing other alignment states surrounded by hairpin defects and lightning defects, This other alignment state is surrounded by these defects that occur in the order of lightening defects and hairpin defects along the uniaxial alignment processing direction, and the ferroelectric liquid crystal in the main alignment state has at least two stable states. shows, the liquid crystal element and their is a half of the angle between the optical axis theta a and ferroelectric liquid crystal tilt angle theta is represented by Θ> θ a> Θ / 2 , and, different polarities A scan signal formed from two phases, a left phase and a write phase, in which the absolute value of the voltage value applied to the pixel in the erase phase is larger than the absolute value of the voltage value applied to the pixel in the write phase A liquid crystal device comprising: means for applying a voltage to a group.
一軸性配向処理が施された一対の基板であって該一軸性
配向処理を同一方向とした一対の基板と、その基板間に
配置された強誘電性液晶とを有し、強誘電性液晶の主た
る配向状態は、この基板間の異物によってまたは基板に
歪みを加えることによってヘアピン欠陥およびライトニ
ング欠陥に囲まれた他の配向状態を生じ、この他の配向
状態は、一軸性配向処理方向に沿ってライトニング欠陥
およびヘアピン欠陥の順序で生じるこれら欠陥により囲
まれたものであり、前記主たる配向状態における強誘電
性液晶が少なくとも2つの安定状態を示し、それらの光
学軸のなす角を2等分する位置に一方の偏光板の吸収軸
を合わせ、それに垂直に他方の偏光板の吸収軸を合わせ
た配置から一方の偏光板だけを時計方向に3°〜30°回
転させたときの第1の安定状態の呈する色と、反時計方
向に同じ角度回転させたときの第2の安定状態の呈する
色が同じである液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。10. A pair of substrates provided with a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment process, wherein the pair of substrates have the uniaxial alignment process in the same direction, and are disposed between the substrates. Having a ferroelectric liquid crystal, the main alignment state of the ferroelectric liquid crystal is caused by foreign substances between the substrates or by applying a strain to the substrate, causing other alignment states surrounded by hairpin defects and lightning defects, The other alignment state is surrounded by these defects that occur in the order of lightening defects and hairpin defects along the uniaxial alignment processing direction, and the ferroelectric liquid crystal in the main alignment state has at least two stable states. Shown, the absorption axis of one of the polarizing plates is aligned with the position at which the angle between the optical axes is divided into two equal parts, and the absorption axis of the other polarizing plate is aligned vertically with the absorption axis of the other polarizing plate. A liquid crystal in which the color in the first stable state when only the light plate is rotated clockwise by 3 ° to 30 ° is the same as the color in the second stable state when rotated by the same angle in the counterclockwise direction. An element, and an absolute value of a voltage value applied to the pixel of the writing phase formed from two phases of an erasing phase and a writing phase having different polarities, and the absolute value of the voltage value applied to the pixel of the erasing phase is determined. A liquid crystal device, comprising: means for applying a larger scanning signal to a scanning electrode group.
一軸性配向処理が施された一対の基板であって該一軸性
配向処理を同一方向とした一対の基板と、その基板間に
配置された強誘電性液晶とを有し、強誘電性液晶の主た
る配向状態は、この基板間の異物によってまたは基板に
歪みを加えることによってヘアピン欠陥およびライトニ
ング欠陥に囲まれた他の配向状態を生じ、この他の配向
状態は、一軸性配向処理方向に沿ってライトニング欠陥
およびヘアピン欠陥の順序で生じるこれら欠陥により囲
まれたものであり、前記主たる配向状態における強誘電
性液晶はクロスニコル下、消光位の透過率の低い2つの
安定状態と、クロスニコル下、消光位の透過率の高い1
つまたは2つの安定状態の計3または4状態を有する液
晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。11. A pair of substrates provided with a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment process, wherein the pair of substrates have the uniaxial alignment process in the same direction, and are disposed between the substrates. Having a ferroelectric liquid crystal, the main alignment state of the ferroelectric liquid crystal is caused by foreign substances between the substrates or by applying a strain to the substrate, causing other alignment states surrounded by hairpin defects and lightning defects, The other alignment state is surrounded by these defects that occur in the order of lightening defects and hairpin defects along the uniaxial alignment processing direction, and the ferroelectric liquid crystal in the main alignment state is under crossed Nicols, and has an extinction position. Two stable states with low transmittance and one with high transmittance in the extinction position under crossed Nicols
A liquid crystal element having a total of three or four states in one or two stable states, and an absolute value of a voltage value formed of two phases of an erasing phase and a writing phase having polarities different from each other and applied to a pixel having the erasing phase A means for applying a scanning signal larger than the absolute value of the voltage value applied to the pixel of the writing phase to the scanning electrode group.
光位の透過率の低い第1と第2の2つの安定状態と、ク
ロスニコル下、消光位の透過率の高い第3と第4の2つ
の安定状態の4つの安定状態を示し、それらの光学軸の
なす角を2等分する位置に一方の偏光板の吸収軸を合わ
せ、それに垂直に他方の偏光板の吸収軸を合わせた配置
から一方の偏光板だけを時計方向に3°〜30°回転させ
たときの第1の安定状態の呈する色と、反時計方向に同
じ角度回転させたときの第2の安定状態の呈する色が同
じであり、一方の偏光板だけを時計方向に3°〜30°回
転させたときの第3の安定状態の呈する色と、反時計方
向に同じ角度回転させたときの第4の安定状態の呈する
色が異なることを特徴とする請求項11記載の液晶装置。12. The first and second stable states in which the ferroelectric liquid crystal has a low transmittance at an extinction position under crossed Nicols, and the third and fourth stable states have a high transmittance at an extinction position under crossed Nicols. The four stable states of the above two are shown, and the absorption axis of one polarizing plate is aligned with the position where the angle between the optical axes is divided into two equal parts, and the absorption axis of the other polarizing plate is aligned perpendicularly thereto. The color in the first stable state when only one of the polarizers is rotated clockwise by 3 ° to 30 ° from the arrangement, and the color in the second stable state when rotated by the same angle in the counterclockwise direction Are the same, and the color of the third stable state when only one of the polarizing plates is rotated clockwise by 3 ° to 30 °, and the fourth stable state when rotated by the same angle in the counterclockwise direction 12. The liquid crystal device according to claim 11, wherein the liquid crystal device has different colors.
一軸性配向処理が施された一対の基板と、その基板間に
配置された強誘電性液晶とを有し、強誘電性液晶は、配
向状態がSmA相を示す高温域からSm*C相を示す温度域に
降温する過程でライトニング欠陥および/またはヘアピ
ン欠陥の発生を伴う配向変化がなく、かつ該配向状態に
おける強誘電性液晶が少なくとも2つの安定状態を示
し、それらの光学軸のなす角度の1/2であるθaと該強誘
電性液晶のチルト角Θとが Θ>θa>Θ/2 で表わされる液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。13. A ferroelectric liquid crystal comprising a pair of substrates having a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment treatment, and a ferroelectric liquid crystal disposed between the substrates. In the process of lowering the temperature from a high temperature region showing the SmA phase to a temperature region showing the Sm * C phase, there is no alignment change accompanied by the occurrence of lightning defects and / or hairpin defects, and at least the ferroelectric liquid crystal in the alignment state shows two stable states, the liquid crystal device and theta a and ferroelectric properties tilt angle of the liquid crystal theta is half the angle between the optical axes thereof are represented by Θ> θ a> Θ / 2 , and, A scan formed from two phases of an erasing phase and a writing phase having different polarities, wherein the absolute value of the voltage value applied to the pixel in the erasing phase is larger than the absolute value of the voltage value applied to the pixel in the writing phase Means for applying signals to the scanning electrode group A liquid crystal device characterized by.
一軸性配向処理が施された一対の基板と、その基板間に
配置された強誘電性液晶とを有し、強誘電性液晶は、配
向状態がSmA相を示す高温域からSm*C相を示す温度域に
降温する過程でライトニング欠陥および/またはヘアピ
ン欠陥の発生を伴う配向変化がなく、かつ該配向状態に
おける強誘電性液晶が少なくとも2つの安定状態を示
し、それらの光学軸のなす角を2等分する位置に一方の
偏光板の吸収軸を合わせ、それに垂直に他方の偏光板の
吸収軸を合わせた配置から一方の偏光板だけを時計方向
に3°〜30°回転させたときの第1の安定状態の呈する
色と、反時計方向に同じ角度回転させたときの第2の安
定状態の呈する色が同じである液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。14. A semiconductor device comprising: a pair of substrates provided with a scanning electrode group and an information electrode group, each of which is subjected to a uniaxial alignment treatment; and a ferroelectric liquid crystal disposed between the substrates. In the process of lowering the temperature from a high temperature region showing the SmA phase to a temperature region showing the Sm * C phase, there is no alignment change accompanied by the occurrence of lightning defects and / or hairpin defects, and at least the ferroelectric liquid crystal in the alignment state The two stable states are shown, and the absorption axis of one of the polarizing plates is aligned at a position bisecting the angle formed by the optical axes, and the absorption axis of the other polarizing plate is aligned perpendicularly to the one polarizing plate. A liquid crystal element having the same color as that of the first stable state when it is rotated clockwise by 3 ° to 30 °, and the same color that the second stable state when it is rotated counterclockwise by the same angle. , And erasure phases of different polarities A scan signal formed from the two phases of the write phase and a write signal in which the absolute value of the voltage value applied to the pixel in the erase phase is larger than the absolute value of the voltage value applied to the pixel in the write phase is applied to the scan electrode group. A liquid crystal device comprising: means for applying voltage.
一軸性配向処理が施された一対の基板と、その基板間に
配置された強誘電性液晶とを有し、強誘電性液晶は、配
向状態がSmA相を示す高温域からSm*C相を示す温度域に
降温する過程でライトニング欠陥および/またはヘアピ
ン欠陥の発生を伴う配向変化がなく、かつ該配向状態に
おける強誘電性液晶がクロスニコル下、消光位の透過率
の低い2つの安定状態と、クロスニコル下、消光位の透
過率の高い1つまたは2つの安定状態の計3または4状
態を有する液晶素子、 並びに、互いに極性の異なる消去位相と書き込み位相の
2つの位相から形成され、該消去位相の画素に印加され
る電圧値の絶対値が該書き込み位相の画素に印加される
電圧値の絶対値よりも大きい走査信号を走査電極群に印
加する手段 を有することを特徴とする液晶装置。15. A ferroelectric liquid crystal comprising: a pair of substrates each having a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment treatment, and a ferroelectric liquid crystal disposed between the substrates. In the process of lowering the temperature from the high temperature region where the alignment state shows the SmA phase to the temperature region showing the Sm * C phase, there is no alignment change accompanied by the occurrence of lightning defects and / or hairpin defects, and the ferroelectric liquid crystal in the alignment state crosses. A liquid crystal element having a total of 3 or 4 states under Nicol and two stable states with low transmittance at the extinction position and one or two stable states under crossed Nicols with high transmittance at the extinction position; Scanning a scanning signal formed from two phases of different erasing phase and writing phase, wherein the absolute value of the voltage value applied to the pixel of the erasing phase is larger than the absolute value of the voltage value applied to the pixel of the writing phase For electrode group A liquid crystal device comprising: means for applying voltage.
光位の透過率の低い第1と第2の2つの安定状態と、ク
ロスニコル下、消光位の透過率の高い第3と第4の2つ
の安定状態の4つの安定状態を示し、それらの光学軸の
なす角を2等分する位置に一方の偏光板の吸収軸を合わ
せ、それに垂直に他方の偏光板の吸収軸を合わせた配置
から一方の偏光板だけを時計方向に3°〜30°回転させ
たときの第1の安定状態の呈する色と、反時計方向に同
じ角度回転させたときの第2の安定状態の呈する色が同
じであり、一方の偏光板だけを時計方向に3°〜30°回
転させたときの第3の安定状態の呈する色と、反時計方
向に同じ角度回転させたときの第4の安定状態の呈する
色が異なることを特徴とする請求項15記載の液晶装置。16. The ferroelectric liquid crystal has first and second stable states having low transmittance at an extinction position under crossed Nicols, and third and fourth stable states having high transmittance at an extinction position under crossed Nicols. The four stable states of the above two are shown, and the absorption axis of one polarizing plate is aligned with the position where the angle between the optical axes is divided into two equal parts, and the absorption axis of the other polarizing plate is aligned perpendicularly thereto. The color in the first stable state when only one of the polarizers is rotated clockwise by 3 ° to 30 ° from the arrangement, and the color in the second stable state when rotated by the same angle in the counterclockwise direction Are the same, and the color of the third stable state when only one of the polarizing plates is rotated clockwise by 3 ° to 30 °, and the fourth stable state when rotated by the same angle in the counterclockwise direction 16. The liquid crystal device according to claim 15, wherein the color of the liquid crystal is different.
ヘアピン欠陥を介さない3つまたは4つの異なる安定状
態を有する請求項1〜3,13〜15のいずれか1項記載の液
晶装置。17. The liquid crystal device according to claim 1, wherein the alignment state has three or four different stable states that do not involve a lightning defect and a hairpin defect.
30°である請求項1〜3のいずれかに記載の液晶装置。18. A pre-tilt angle α of the liquid crystal is 6 ° <α <
The liquid crystal device according to claim 1, wherein the angle is 30 °.
30°である請求項1〜3のいずれかに記載の液晶装置。19. A pretilt angle α of the liquid crystal is 8 ° <α <
The liquid crystal device according to claim 1, wherein the angle is 30 °.
30°である請求項1〜3のいずれかに記載の液晶装置。20. A pretilt angle α of the liquid crystal is 10 ° <α <
The liquid crystal device according to claim 1, wherein the angle is 30 °.
6°<α<30°である請求項5〜16のいずれかに記載の
液晶装置。21. When the pretilt angle of the liquid crystal is α,
The liquid crystal device according to claim 5, wherein 6 ° <α <30 °.
8°<α<30°である請求項5〜16のいずれかに記載の
液晶装置。22. When the pretilt angle of the liquid crystal is α,
The liquid crystal device according to claim 5, wherein 8 ° <α <30 °.
10°<α<30°である請求項5〜16のいずれかに記載の
液晶装置。23. When the pretilt angle of the liquid crystal is α,
The liquid crystal device according to claim 5, wherein 10 ° <α <30 °.
°である請求項1〜3のいずれかに記載の液晶装置。24. The tilt angle Θ of the liquid crystal is 7 ° <Θ <27.
The liquid crystal device according to claim 1, wherein the angle is °.
<27°である請求項5〜16のいずれかに記載の液晶装
置。25. When the tilt angle of the liquid crystal is Θ, 7 ° <Θ.
The liquid crystal device according to claim 5, wherein the angle is <27 °.
一軸性配向処理が施こされた一対の基板と、 前記基板間に配置されたカイラルスメクチック液晶とを
有し、 前記カイラルスメクチック液晶のプレチルト角をα、チ
ルト角をΘ、カイラルスメクチック層の基板法線に対す
る傾斜角をδとした時、カイラルスメクチック液晶は、 Θ<α+δ で表わされる配向状態を有し、かつ該配向状態における
カイラルスメクチック液晶が少なくとも2つの安定状態
を示し、それらの光学軸のなす角度の1/2であるθaと該
液晶のチルト角Θとが Θ>θa>Θ/2 の関係を有する液晶素子と、 互いに極性の異なる消去位相と書き込み位相の2つの位
相から形成され、該消去位相の画素に印加される電圧値
の絶対値が該書き込み位相の画素に印加される電圧値よ
りも大きい走査信号を走査電極群に印加する手段とを有
することを特徴とする液晶装置。26. A pretilt of the chiral smectic liquid crystal, comprising: a pair of substrates provided with a scanning electrode group and an information electrode group, each of which has been subjected to a uniaxial alignment treatment; and a chiral smectic liquid crystal disposed between the substrates. When the angle is α, the tilt angle is Θ, and the tilt angle of the chiral smectic layer with respect to the substrate normal is δ, the chiral smectic liquid crystal has an alignment state represented by Θ <α + δ, and the chiral smectic liquid crystal in the alignment state There exhibits at least two stable states, a liquid crystal element having those is 1/2 of the angle of the optical axis theta a and the liquid crystal and the tilt angle theta is Θ> θ a> Θ / 2 in relation to each other It is formed from two phases of erase phase and write phase having different polarities, and the absolute value of the voltage value applied to the pixel at the erase phase is larger than the voltage value applied to the pixel at the write phase. A liquid crystal device characterized in that it comprises a means for applying a listening scan signal to the scan electrode group.
ルト角αが、6°<α<30°である請求項26記載の液晶
装置。27. The liquid crystal device according to claim 26, wherein a pretilt angle α of the chiral smectic liquid crystal satisfies 6 ° <α <30 °.
角Θが、7°<Θ<27°である請求項26記載の液晶装
置。28. The liquid crystal device according to claim 26, wherein the tilt angle の of the chiral smectic liquid crystal is 7 ° <Θ <27 °.
ルト角αと傾斜角δの関係が、δ<αで表される配向状
態を有する請求項26記載の液晶装置。29. The liquid crystal device according to claim 26, wherein the relationship between the pretilt angle α and the tilt angle δ of the chiral smectic liquid crystal has an alignment state represented by δ <α.
配向処理がラビング処理である請求項1〜29記載の液晶
装置。30. The liquid crystal device according to claim 1, wherein the uniaxial alignment treatment performed on each of the pair of substrates is a rubbing treatment.
グ処理の方向が、互いに20°以下の角度をなすようにク
ロスしている請求項30記載の液晶装置。31. The liquid crystal device according to claim 30, wherein the rubbing directions applied to each of the pair of substrates cross each other so as to form an angle of 20 ° or less.
Priority Applications (10)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2090414A JP2612504B2 (en) | 1990-04-06 | 1990-04-06 | Liquid crystal device |
EP91103125A EP0444705B1 (en) | 1990-03-02 | 1991-03-01 | Liquid crystal element and liquid crystal apparatus using the same |
DE69131258T DE69131258T2 (en) | 1990-03-02 | 1991-03-01 | Liquid crystal element and liquid crystal device using this element |
US07/663,436 US5189536A (en) | 1990-03-02 | 1991-03-01 | Ferroelectric liquid crystal element having uniform high temperature alignment |
AT91103125T ATE180580T1 (en) | 1990-03-02 | 1991-03-01 | LIQUID CRYSTAL ELEMENT AND LIQUID CRYSTAL DEVICE USING SUCH ELEMENT |
EP98119023A EP0886173A3 (en) | 1990-03-02 | 1991-03-01 | Liquid crystal element and liquid crystal apparatus using the same |
AU72047/91A AU634031B2 (en) | 1990-03-02 | 1991-03-01 | Liquid crystal element and liquid crystal apparatus using the same |
KR1019910003441A KR940005123B1 (en) | 1990-03-02 | 1991-03-02 | Liquid crystal display device using liquid crystal device |
US08/272,652 US5481387A (en) | 1990-03-02 | 1994-07-11 | Chiral smectic liquid crystal element having uniform high temperature alignment and α≧8 degrees |
US08/527,775 US6456349B1 (en) | 1990-03-02 | 1995-09-13 | Liquid crystal element and liquid crystal apparatus using the same |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2090414A JP2612504B2 (en) | 1990-04-06 | 1990-04-06 | Liquid crystal device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH03288825A JPH03288825A (en) | 1991-12-19 |
JP2612504B2 true JP2612504B2 (en) | 1997-05-21 |
Family
ID=13997936
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2090414A Expired - Fee Related JP2612504B2 (en) | 1990-03-02 | 1990-04-06 | Liquid crystal device |
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JP (1) | JP2612504B2 (en) |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61267739A (en) * | 1986-02-03 | 1986-11-27 | Canon Inc | Method for driving optical modulating element |
JPH03243920A (en) * | 1990-02-22 | 1991-10-30 | Seiko Epson Corp | Liquid crystal electrooptical device |
-
1990
- 1990-04-06 JP JP2090414A patent/JP2612504B2/en not_active Expired - Fee Related
Also Published As
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JPH03288825A (en) | 1991-12-19 |
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