JPH095708A - Liquid crystal display device and its driving method - Google Patents

Liquid crystal display device and its driving method

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Publication number
JPH095708A
JPH095708A JP15204895A JP15204895A JPH095708A JP H095708 A JPH095708 A JP H095708A JP 15204895 A JP15204895 A JP 15204895A JP 15204895 A JP15204895 A JP 15204895A JP H095708 A JPH095708 A JP H095708A
Authority
JP
Japan
Prior art keywords
liquid crystal
scanning
stable state
state
display device
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP15204895A
Other languages
Japanese (ja)
Inventor
Yutaka Inaba
豊 稲葉
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Canon Inc
Original Assignee
Canon Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Canon Inc filed Critical Canon Inc
Priority to JP15204895A priority Critical patent/JPH095708A/en
Priority to US08/665,947 priority patent/US6061045A/en
Publication of JPH095708A publication Critical patent/JPH095708A/en
Pending legal-status Critical Current

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  • Liquid Crystal (AREA)

Abstract

PURPOSE: To provide an antiferroelectric liquid crystal display device having high quality free from flickering. CONSTITUTION: This liquid crystal display device has a display panel which has matrix pixels formed by intersection of scanning signal electrodes 111 to 116 and information signal electrodes 121 to 126 orthogonal with each other, ferroelectric liquid crystals which exist in the spacing between the two electrodes and attain a first stable state consisting of an antiferroelectric phase at the time of non-electric field and a second or third stable state consisting of a ferroelectric phase according to the polarities of electric fields at the time of impression of the electric fields and a polarizing device which puts the first stable state into a dark state and the second and third states into a bright state. The display device is so constituted that the scanning of the scanning signal electrodes is executed by interlaced scanning of every other piece and that the polarities of the selection voltage to be impressed on the liquid crystals are inverted at every one horizontal period of the scanning.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、反強誘電相と強誘電相
とを取る強誘電性液晶を用いた液晶表示装置及びその駆
動方法に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a liquid crystal display device using a ferroelectric liquid crystal having an antiferroelectric phase and a ferroelectric phase, and a driving method thereof.

【0002】[0002]

【従来の技術】電界によって3つの光学状態を取る液晶
表示装置が特開平2−153322号、特開平2−17
3724号などに開示されている。その後これが液晶の
反強誘電性によるものであることがChandani等
(ジャパニーズ・ジャーナル・オブ・アプライド・フィ
ジクス28巻(1989)L1265頁)によって明ら
かにされた。
2. Description of the Related Art Liquid crystal display devices that take three optical states by an electric field are disclosed in Japanese Patent Laid-Open Nos. 2-153322 and 2-17.
No. 3724 and the like. It was subsequently revealed by Chandani et al. (Japanese Journal of Applied Physics 28 (1989) L1265 page) that this is due to the antiferroelectricity of liquid crystals.

【0003】それによると、反強誘電性を示す強誘電性
液晶(以下、反強誘電性液晶という。)は通常の強誘電
性液晶と同じく薄い基板間隙中でらせんが解けて、図4
(a)に示すように無電界時(E=0)には液晶分子が
スメクティック層毎に反対方向にチルトした構造をと
り、そのため無電界時には光軸は層法線方向を向く。
According to this, a ferroelectric liquid crystal exhibiting antiferroelectricity (hereinafter referred to as an antiferroelectric liquid crystal) unwinds a spiral in a thin substrate gap as in a normal ferroelectric liquid crystal, and FIG.
As shown in (a), when there is no electric field (E = 0), liquid crystal molecules are tilted in opposite directions for each smectic layer. Therefore, when there is no electric field, the optical axis is oriented in the layer normal direction.

【0004】電界印加(E>0、E<0)によって強誘
電相への転移が起こり、液晶分子がすべての層で電界の
方向によって決まる同一方向にチルトした構造をとる結
果、光軸は層法線から傾き層法線に対して対称な2つの
方向のいずれかになる。これを図4(b),(c)に示
した。
The transition to the ferroelectric phase occurs due to the application of an electric field (E> 0, E <0), and the liquid crystal molecules have a structure in which all layers are tilted in the same direction determined by the direction of the electric field. It is one of two directions that are symmetric from the normal to the tilted layer normal. This is shown in FIGS. 4 (b) and 4 (c).

【0005】この反強誘電性液晶を表示装置に応用する
場合は通常2枚の偏光板で挟み、図4中に両矢印線で示
したように偏光板の吸収軸を層法線に平行および垂直
に、2枚の偏光板がクロスニコルとなるように配置す
る。この配置では、無電界時の反強誘電状態が暗状態、
電界印加時の強誘電状態が明状態となる。
When this antiferroelectric liquid crystal is applied to a display device, it is usually sandwiched between two polarizing plates, and the absorption axis of the polarizing plate is parallel to the layer normal as indicated by the double-headed arrow line in FIG. The two polarizing plates are arranged vertically so as to form a crossed Nicols. In this arrangement, the antiferroelectric state when there is no electric field is the dark state,
The ferroelectric state when the electric field is applied becomes the bright state.

【0006】この配置の特徴は明状態が2通りあること
で、これを利用して一定周期ごとに明状態の印加電圧極
性を切り替える方法が上記特開平2−173724号に
開示されている。該発明は単純マトリクス構成での反強
誘電性液晶装置の発明であって図5にその駆動波形の一
例を示す。
The feature of this arrangement is that there are two bright states, and a method of switching the polarity of the applied voltage in the bright state at regular intervals using this is disclosed in Japanese Patent Laid-Open No. 2-173724. The present invention is an invention of an antiferroelectric liquid crystal device having a simple matrix structure, and FIG. 5 shows an example of its drive waveform.

【0007】図5は液晶にかかる電圧の時間変動の様子
を示すもので、フレームごとに画素に印加される電圧の
極性が入れ替わっている。図5から明らかなとおり液晶
にかかる電圧は時間的に平均化されて0になる。これに
よりDC電圧成分による液晶の劣化を防止できるという
利点がある。
FIG. 5 shows how the voltage applied to the liquid crystal changes with time, and the polarities of the voltages applied to the pixels are exchanged for each frame. As is clear from FIG. 5, the voltage applied to the liquid crystal is averaged over time and becomes zero. This has the advantage of preventing deterioration of the liquid crystal due to the DC voltage component.

【0008】[0008]

【発明が解決しようとする課題】しかしながら、上記フ
レーム毎の極性反転駆動法には欠点があって、それは表
示パネルを斜めから見たときに画面がちらつくという点
である。その理由を以下に示す。
However, the polarity inversion driving method for each frame has a drawback in that the screen flickers when the display panel is viewed obliquely. The reason is shown below.

【0009】図6は表示パネルを右斜め下から見たとき
の液晶分子と上下の偏光板の透過軸とを示したもので
る。(a)は暗状態、(b),(c)は2つの明状態
で、それぞれを正面から見たものが図4(a),
(b),(c)に対応する。
FIG. 6 shows liquid crystal molecules and the transmission axes of the upper and lower polarizing plates when the display panel is viewed from diagonally lower right. 4A shows a dark state, and FIGS. 4B and 4C show two bright states.
It corresponds to (b) and (c).

【0010】(b)と(c)をくらべると(b)では液
晶分子をほぼ真横から見ているので実効的な屈折率異方
性は正面から見た場合とあまり違わないのに対し、
(c)では液晶分子をその長軸近くから見ていることに
なり、正面から見るのと比べて屈折率異方性が著しく小
さくなる。そのために(b)と(c)では透過率に差が
生じ、これがフレームごとに切り替わるのでちらつきと
して見えるのである。
Comparing (b) and (c), in (b), the liquid crystal molecules are viewed almost from the side, so the effective refractive index anisotropy is not much different from that when viewed from the front.
In (c), the liquid crystal molecules are viewed from the vicinity of their major axes, and the refractive index anisotropy is significantly smaller than when viewed from the front. Therefore, there is a difference in transmittance between (b) and (c), and this is switched for each frame, so that it appears as a flicker.

【0011】さらに斜めから見ると光路長が長くなるの
で(b)の場合リタデーションが最適値からずれ、黄色
く色づいて見えるのもちらつきの一因である。
Further, since the optical path length becomes long when viewed obliquely, in the case of (b), the retardation deviates from the optimum value, which is one of the causes of the flicker that the yellow color appears.

【0012】このような素子をマトリクス配列させた表
示装置を考える。通常、テレビ画像などを表示する際に
は、走査線を1本ずつ飛び越して選択するいわゆるイン
タレース走査が行われる。このときの各フレーム毎の画
素の状態を表したのが図7(a)〜(d)である。
Consider a display device in which such elements are arranged in a matrix. Generally, when displaying a television image or the like, so-called interlaced scanning is performed in which scanning lines are skipped one by one and selected. FIGS. 7A to 7D show the states of the pixels in each frame at this time.

【0013】図7において、511、512、513、
・・・は走査電極、521、522、623、・・・は
信号電極、53は画素である。画素の中の短い線分はそ
の画素での液晶の光軸方向を表したもので、情報信号線
に平行なものは反強誘電状態(暗)、傾いているものは
強誘電状態(明)を示す。なお、ここでは便宜上、信号
線を法線方向として置くが、これは必ずしも必要ではな
く任意の方向であってよい。右に傾いた状態は正極性電
圧によって、左に傾いた状態は負極性電圧によって書き
込まれたものとする。これは自発分極の符合で決まって
いるので液晶に依存する。54、55は上下の偏光板の
軸方向である。
In FIG. 7, 511, 512, 513,
Is a scanning electrode, 521, 522, 623, ... Is a signal electrode, and 53 is a pixel. The short line segment in a pixel represents the direction of the optical axis of the liquid crystal in that pixel. Those parallel to the information signal line are in the antiferroelectric state (dark), and those that are inclined are in the ferroelectric state (bright). Indicates. Note that, here, for convenience, the signal line is set as the normal direction, but this is not necessarily required and may be an arbitrary direction. It is assumed that the state of leaning to the right is written by a positive voltage and the state of leaning to the left is written by a negative voltage. This depends on the liquid crystal because it is determined by the sign of spontaneous polarization. 54 and 55 are the axial directions of the upper and lower polarizing plates.

【0014】画素が全て明状態にあるとして、あるフレ
ームで図7(a)のようになったとする。これは正電圧
によって書き込まれた状態である。ここでは奇数番の走
査電極が負電圧選択インタレース走査されたとするとそ
の結果は図7(b)になる。次いで、偶数走査電極の負
電圧インタレース走査が行われ、その結果図7(c)に
なり、また奇数走査電極の正電圧インタレース走査が行
われるから図7(d)になる。その次の偶数インタレー
ス走査によって図7(a)に戻り以下同じサイクルが繰
り返される。すなわち、4フレームを1つの周期として
分子配列状態が変化するので、透過率変動の周波数が低
くちらつきが著しい。
It is assumed that all the pixels are in a bright state and a certain frame has a state as shown in FIG. This is the state written by the positive voltage. Here, if the odd-numbered scan electrodes are subjected to negative voltage selective interlace scanning, the result is shown in FIG. 7B. Next, a negative voltage interlaced scan of the even scan electrodes is performed, resulting in FIG. 7C, and a positive voltage interlaced scan of the odd scan electrodes results in FIG. 7D. The next even interlaced scan returns to FIG. 7A, and the same cycle is repeated thereafter. That is, since the molecular arrangement state changes with 4 frames as one cycle, the frequency of transmittance fluctuation is low and flicker is significant.

【0015】本発明は、ちらつきのない高品質の反強誘
電性液晶表示装置を提供することを目的としている。
It is an object of the present invention to provide a high quality anti-ferroelectric liquid crystal display device without flicker.

【0016】[0016]

【課題を解決するための手段】本発明は、互いに直交す
る走査信号電極と情報信号電極の交差によって形成され
たマトリクス画素を有する表示パネルと、前記2つの電
極の間隙にあって、無電界時に反強誘電相からなる第1
の安定状態を取り、電界印可時に電界の極性に応じて強
誘電相からなる第2又は第3の安定状態を取る強誘電性
液晶と、上記第1の安定状態を暗状態、第2及び第3の
状態を明状態とする偏光装置とを備える液晶表示装置に
おいて、前記走査信号電極の走査を1本づつの飛び越し
走査で行うと共に、該走査の1水平期間ごとに液晶に印
可する選択電圧の極性を反転させるように構成したこと
を特徴としている。
According to the present invention, there is provided a display panel having a matrix pixel formed by intersections of scanning signal electrodes and information signal electrodes which are orthogonal to each other, and in a gap between the two electrodes, there is no electric field. First composed of antiferroelectric phase
And a ferroelectric liquid crystal that takes a second or third stable state consisting of a ferroelectric phase according to the polarity of the electric field when an electric field is applied, and the first stable state is the dark state, the second and the third stable state. In a liquid crystal display device including a polarizing device for turning the state 3 into a bright state, scanning of the scanning signal electrodes is performed by interlaced scanning one by one, and the selection voltage applied to the liquid crystal is applied every horizontal period of the scanning. It is characterized in that the polarity is reversed.

【0017】また、本発明は、互いに直交する走査信号
電極と情報信号電極の交差によって形成されたマトリク
ス画素を有する表示パネルと、前記2つの電極の間隙に
あって、無電界時に反強誘電相からなる第1の安定状態
を取り、電界印可時に電界の極性に応じて強誘電相から
なる第2又は第3の安定状態を取る強誘電性液晶と、上
記第1の安定状態を暗状態、第2及び第3の安定状態を
明状態とする偏光装置とを備える液晶表示装置の駆動方
法において、前記走査信号電極の走査を1本づつの飛び
越し走査で行うと共に、該走査の1水平期間ごとに液晶
に印可する選択電圧の極性を反転させるようにしたこと
を特徴としている。
Further, according to the present invention, there is provided a display panel having a matrix pixel formed by intersections of scanning signal electrodes and information signal electrodes which are orthogonal to each other, and an antiferroelectric phase in a gap between the two electrodes when no electric field is applied. A ferroelectric liquid crystal that takes a first stable state consisting of a ferroelectric liquid crystal that takes a second or third stable state consisting of a ferroelectric phase according to the polarity of the electric field when an electric field is applied, and the first stable state is a dark state, In a method of driving a liquid crystal display device, comprising: a polarizing device for turning a second and a third stable state into a bright state, scanning of the scanning signal electrodes is performed by interlaced scanning one by one, and every one horizontal period of the scanning. In addition, the polarity of the selection voltage applied to the liquid crystal is reversed.

【0018】[0018]

【作用】本発明は、上述のように構成されているので、
例えば表示面が明状態とすると、走査ラインは2本づつ
第2の安定状態か第3の安定状態になり、分子配列が2
列ずつ交互に並んでいるので透過率や色づきなどが平均
化され相互の区別が付かず、ちらつきが著しく少なくな
る。
Since the present invention is constructed as described above,
For example, when the display surface is in the bright state, the scanning lines are set to the second stable state or the third stable state for every two lines, and the molecular arrangement becomes 2
Since the columns are alternately arranged, the transmittance and coloring are averaged, and they are not distinguished from each other, and the flicker is significantly reduced.

【0019】[0019]

【実施例】以下、図面に基づき本発明の実施例について
説明する。
Embodiments of the present invention will be described below with reference to the drawings.

【0020】図1は、本発明の実施例によって表示され
る表示パネル面の模式図で、図中の111、112、1
13、114、115、116は走査電極を、121、
122、123、124、125、126は信号電極
を、短線13は液晶分子の光軸方向を示しており、
(a)は初期状態を示している。但し、表示面は明状態
となっている。
FIG. 1 is a schematic view of a display panel surface displayed according to an embodiment of the present invention.
Reference numerals 13, 114, 115 and 116 denote scan electrodes, 121 and
122, 123, 124, 125, 126 are signal electrodes, and the short line 13 is the optical axis direction of liquid crystal molecules.
(A) has shown the initial state. However, the display surface is in a bright state.

【0021】ここで、奇数走査線のインタレース走査と
して、第1、5、9、13、・・・(一般に4k+1、
kは整数)本目の走査線は正極性の書き込み、第3、
7、11、15、・・・(一般に4k+3)本面の走査
線は負極性の書き込みとなるように選択走査すると、結
果は図1(b)のようになる。
Here, as interlaced scanning of odd-numbered scanning lines, the first, fifth, ninth, thirteenth, ... (Generally, 4k + 1,
(k is an integer) The third scanning line is the positive writing, the third,
1, 11, 15, ... (Generally 4k + 3) The scanning lines on the main surface are selectively scanned so that the writing is of negative polarity, and the result is as shown in FIG.

【0022】つぎに、偶数走査線のインタレース走査と
して、第2、6、10、14、・・・(一般に4k+
2、kは整数)本目の走査線は正極性の書き込み、第
4、8、12、16、・・・(一般に4k)本面の走査
線は負極性の書き込みとなるように選択走査すると、結
果は図1(c)のようになる。
Next, as an interlaced scan of even scan lines, the second, sixth, tenth, 14, ... (Generally 4k +
(2, k is an integer) When the selective scanning is performed such that the scanning line of the fourth scanning line is for positive polarity writing and the scanning lines of the fourth, eighth, 12, 16, ... (Generally 4k) scanning lines are for negative polarity writing, The result is as shown in FIG.

【0023】次いで、奇数インタレース走査を先の場合
とは逆極性に、第1、5、9、13、・・・本目の走査
線は負極性の書き込み、第3、7、11、15、・・・
本面の走査線は正極性の書き込みとなるように選択走査
すると、結果は図1(d)のようになる。
Next, odd-numbered interlaced scanning is performed in the opposite polarity to that of the previous case, and the first, fifth, ninth, thirteenth, ... Scanning lines are written in the negative polarity, third, seventh, 11, 15 ,. ...
When selective scanning is performed so that the scanning line on the main surface has positive polarity writing, the result is as shown in FIG.

【0024】次に、偶数インタレース走査を先ほどとは
逆極性に、第2、6、10、14、・・・本目の走査線
は負極性の書き込み、第4、8、12、16、・・・本
面の走査線は負極性の書き込みとなるように選択走査す
ると、結果は図1(a)に戻る。
Next, even-numbered interlaced scanning is performed in the opposite polarity to the previous one, and the second, sixth, tenth, fourteenth, ... Scanning lines are written in the negative polarity, the fourth, eighth, 12, 16, ... .. If the scanning line on the main surface is selectively scanned so that the writing is of negative polarity, the result returns to FIG.

【0025】以下この走査を繰り返す。This scanning is repeated thereafter.

【0026】この場合も、表示周期は4フレームで図7
の場合と同じであるが、図1(a)〜(b)はともに2
走査ラインずつ分子配置が交互に並んでいるので透過率
や色づきなどが平均化されて目には相互の区別が付かな
い。
Also in this case, the display cycle is 4 frames as shown in FIG.
1 is the same as that of FIG.
Since the molecular arrangement is alternately arranged for each scanning line, the transmittance and the coloring are averaged and the eyes cannot distinguish each other.

【0027】(a)(c)と(b)(d)とは分子配置
周期が1ラインずれているが、これも平均化のために目
には識別されず、結局図1の場合は1フレームの周期と
して感じられ図7に比べてちらつきの程度が著しく軽減
された。
The molecular arrangement periods of (a) (c) and (b) (d) are shifted by one line, but this is also not discerned by the eye due to averaging, and in the case of FIG. It was felt as a frame cycle, and the degree of flicker was remarkably reduced as compared with FIG. 7.

【0028】図2は、図1に示した表示画面状態にする
ための具体的な駆動波形である。611〜618は走査
電極に印可させる電圧、62は信号電極に印可される電
圧である。
FIG. 2 shows specific drive waveforms for setting the display screen state shown in FIG. Reference numerals 611 to 618 are voltages applied to the scanning electrodes, and 62 is a voltage applied to the signal electrodes.

【0029】走査線選択期間Tの直前に0ボルトのリセ
ット期間Rがあり、ライン上の全画素を暗状態にリセッ
トする。選択後の比選択期間Nには書き込んだ状態維持
するためのDC電圧が印可される。これは従来型(図
5)と同様である。
Immediately before the scanning line selection period T, there is a reset period R of 0 volt, and all the pixels on the line are reset to the dark state. During the ratio selection period N after selection, a DC voltage for maintaining the written state is applied. This is similar to the conventional type (FIG. 5).

【0030】第1、第3フレームでは奇数走査線のみが
選択され、第2、第4フレームでは偶数走査線のみが選
択されている。各フレーム内で一本毎に選択電圧の極性
が反転している。これにより図1で示した表示が得られ
る。
Only odd scan lines are selected in the first and third frames, and only even scan lines are selected in the second and fourth frames. The polarity of the selection voltage is inverted for each line in each frame. As a result, the display shown in FIG. 1 is obtained.

【0031】62の画像信号はHで示される期間が1単
位である。走査線選択電圧との合成電圧が閾値を越える
と画素は明状態になる。62は全ての画素が明状態のも
のである。暗状態は極性を反転したものを与える。
In the image signal 62, the period indicated by H is 1 unit. When the combined voltage with the scanning line selection voltage exceeds the threshold value, the pixel becomes bright. In 62, all pixels are in a bright state. The dark state gives the opposite polarity.

【0032】なお、本実施例で用いる反強誘電性液晶材
料としては、化1に示すものが上げられる。
As the antiferroelectric liquid crystal material used in this embodiment, those shown in Chemical formula 1 can be cited.

【0033】[0033]

【化1】 次に、具体的なセル構成について説明する。Embedded image Next, a specific cell configuration will be described.

【0034】化1で示した液晶を、対向面に電極を形成
した2枚の透明基板の間隙(ギャップ2.5μm)に破
産で表示パネルを製造した。図3に表示パネルの断面を
示す。
A display panel was manufactured by bankruptcy of the liquid crystal shown in Chemical formula 1 in a gap (gap 2.5 μm) between two transparent substrates having electrodes formed on opposite surfaces. FIG. 3 shows a cross section of the display panel.

【0035】一方の基板71は走査電極72が形成され
ており、その上にナイロン薄膜73(厚さ5nm)をラ
ビングした層が覆っている。ナイロンの代わりにポリイ
ミドを用いることができる。
A scanning electrode 72 is formed on one of the substrates 71, and a layer formed by rubbing a nylon thin film 73 (thickness: 5 nm) covers the scanning electrode 72. Polyimide can be used instead of nylon.

【0036】他方の基板74は、信号電極75と、その
上には基板間の短絡防止のため酸化チタンと酸化ジルコ
ニウムの混合膜76が形成されており、更にその上をシ
ロキサンを主成分とする表面処理膜77が厚さ10nm
以下で覆っている。
The other substrate 74 has a signal electrode 75 and a mixed film 76 of titanium oxide and zirconium oxide formed thereon for preventing a short circuit between the substrates, and further has a siloxane as a main component thereon. Surface treatment film 77 has a thickness of 10 nm
Covered below.

【0037】この表面処理膜は対向側のラビング膜に比
べて表面エネルギが小さく、従って液晶をホモジニアス
配向させる力が弱い。そのため、液晶が等方層からの冷
却によってスメクティック層におりてくる際に方向秩序
とスメクティック層秩序がラビング膜面側から優先的に
起こり、両面から無秩序に起こることによって生じる配
向欠陥がなく、結果として均一な配向が得られる。
This surface-treated film has a smaller surface energy than the rubbing film on the opposite side, and therefore has a weak force for homogeneously aligning the liquid crystal. Therefore, when the liquid crystal comes to the smectic layer by cooling from the isotropic layer, the directional order and the smectic layer order occur preferentially from the rubbing film surface side, and there is no alignment defect caused by the disorder occurring from both surfaces. As a result, uniform alignment can be obtained.

【0038】[0038]

【発明の効果】以上説明したように、本発明によると、
走査信号電極の走査を1本づつの飛び越し走査で行うと
共に、該走査の1水平期間ごとに液晶に印可する選択電
圧の極性を反転させるように構成したので、画像のちら
つきが少なくなると共に、斜めから見たときの透過率と
色合いの差もなくなり、全体として視角特性が向上す
る。
As described above, according to the present invention,
Since the scanning of the scanning signal electrodes is performed by interlaced scanning one by one and the polarity of the selection voltage applied to the liquid crystal is inverted every horizontal period of the scanning, the flicker of the image is reduced and the diagonal The difference between the transmittance and the hue when viewed from above is eliminated, and the viewing angle characteristics are improved as a whole.

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

【図1】本発明の実施例を示す図である。FIG. 1 is a diagram showing an embodiment of the present invention.

【図2】図1の表示を行うための駆動波形図である。FIG. 2 is a drive waveform diagram for performing the display of FIG.

【図3】実施例にかかる強誘電性液晶素子の断面図であ
る。
FIG. 3 is a sectional view of a ferroelectric liquid crystal device according to an example.

【図4】反強誘電相と強誘電相の液晶分子配置を示す図
である。
FIG. 4 is a diagram showing an arrangement of liquid crystal molecules in an antiferroelectric phase and a ferroelectric phase.

【図5】従来の液晶駆動波形を示す図である。FIG. 5 is a diagram showing a conventional liquid crystal drive waveform.

【図6】図4の状態を斜めから見た図である。FIG. 6 is a view of the state of FIG. 4 seen obliquely.

【図7】ちらつきが生じる表示面の説明図である。FIG. 7 is an explanatory diagram of a display surface in which flicker occurs.

【符号の説明】[Explanation of symbols]

13 液晶分子の光軸方向 111 走査電極 112 走査電極 113 走査電極 114 走査電極 115 走査電極 116 走査電極 121 信号電極 122 信号電極 123 信号電極 124 信号電極 125 信号電極 126 信号電極 13 Optical axis direction of liquid crystal molecule 111 Scan electrode 112 Scan electrode 113 Scan electrode 114 Scan electrode 115 Scan electrode 116 Scan electrode 121 Signal electrode 122 Signal electrode 123 Signal electrode 124 Signal electrode 125 Signal electrode 126 Signal electrode

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 互いに直交する走査信号電極と情報信号
電極の交差によって形成されたマトリクス画素を有する
表示パネルと、前記2つの電極の間隙にあって、無電界
時に反強誘電相からなる第1の安定状態を取り、電界印
可時に電界の極性に応じて強誘電相からなる第2又は第
3の安定状態を取る強誘電性液晶と、上記第1の安定状
態を暗状態、第2及び第3の安定状態を明状態とする偏
光装置とを備える液晶表示装置において、 前記走査信号電極の走査を1本づつの飛び越し走査で行
うと共に、該走査の1水平期間ごとに液晶に印可する選
択電圧の極性を反転させるように構成したことを特徴と
する液晶表示装置。
1. A display panel having a matrix pixel formed by intersections of scanning signal electrodes and information signal electrodes which are orthogonal to each other, and a first panel formed of an antiferroelectric phase in a gap between the two electrodes when no electric field is applied. And a ferroelectric liquid crystal that takes a second or third stable state consisting of a ferroelectric phase according to the polarity of the electric field when an electric field is applied, and the first stable state is the dark state, the second and the third stable state. In a liquid crystal display device including a polarizing device for turning the stable state of No. 3 into a bright state, the scanning signal electrodes are scanned by interlaced scanning one by one, and a selection voltage applied to the liquid crystal in each horizontal period of the scanning. A liquid crystal display device characterized in that the polarity of the liquid crystal display is reversed.
【請求項2】 互いに直交する走査信号電極と情報信号
電極の交差によって形成されたマトリクス画素を有する
表示パネルと、前記2つの電極の間隙にあって、無電界
時に反強誘電相からなる第1の安定状態を取り、電界印
可時に電界の極性に応じて強誘電相からなる第2又は第
3の安定状態を取る強誘電性液晶と、上記第1の安定状
態を暗状態、第2及び第3の安定状態を明状態とする偏
光装置とを備える液晶表示装置の駆動方法において、 前記走査信号電極の走査を1本づつの飛び越し走査で行
うと共に、該走査の1水平期間ごとに液晶に印可する選
択電圧の極性を反転させるようにしたことを特徴とする
液晶表示装置の駆動方法。
2. A display panel having a matrix pixel formed by intersections of scanning signal electrodes and information signal electrodes orthogonal to each other, and a first antiferroelectric phase in a gap between the two electrodes and having no electric field. And a ferroelectric liquid crystal that takes a second or third stable state consisting of a ferroelectric phase according to the polarity of the electric field when an electric field is applied, and the first stable state is the dark state, the second and the third stable state. In a method of driving a liquid crystal display device including a polarization device for making a stable state into a bright state, the scanning signal electrodes are scanned by interlaced scanning one by one, and the liquid crystal is applied to the liquid crystal every horizontal period of the scanning. A method for driving a liquid crystal display device, characterized in that the polarity of the selection voltage is reversed.
JP15204895A 1995-06-19 1995-06-19 Liquid crystal display device and its driving method Pending JPH095708A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP15204895A JPH095708A (en) 1995-06-19 1995-06-19 Liquid crystal display device and its driving method
US08/665,947 US6061045A (en) 1995-06-19 1996-06-19 Liquid crystal display apparatus and method of driving same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15204895A JPH095708A (en) 1995-06-19 1995-06-19 Liquid crystal display device and its driving method

Publications (1)

Publication Number Publication Date
JPH095708A true JPH095708A (en) 1997-01-10

Family

ID=15531919

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15204895A Pending JPH095708A (en) 1995-06-19 1995-06-19 Liquid crystal display device and its driving method

Country Status (1)

Country Link
JP (1) JPH095708A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6307533B1 (en) 1997-08-21 2001-10-23 Denso Corporation Liquid crystal display device with matrix electrode structure
JP2012042710A (en) * 2010-08-19 2012-03-01 Seiko Epson Corp Liquid crystal drive device, liquid crystal display device, electronic device, and liquid crystal drive method

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6307533B1 (en) 1997-08-21 2001-10-23 Denso Corporation Liquid crystal display device with matrix electrode structure
JP2012042710A (en) * 2010-08-19 2012-03-01 Seiko Epson Corp Liquid crystal drive device, liquid crystal display device, electronic device, and liquid crystal drive method
US9082358B2 (en) 2010-08-19 2015-07-14 Seiko Epson Corporation Liquid crystal driving device, liquid crystal display apparatus, electronic apparatus and liquid crystal driving method

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