JPH03209216A - Liquid crystal element, driving method for the same and liquid crystal display device - Google Patents

Liquid crystal element, driving method for the same and liquid crystal display device

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Publication number
JPH03209216A
JPH03209216A JP416090A JP416090A JPH03209216A JP H03209216 A JPH03209216 A JP H03209216A JP 416090 A JP416090 A JP 416090A JP 416090 A JP416090 A JP 416090A JP H03209216 A JPH03209216 A JP H03209216A
Authority
JP
Japan
Prior art keywords
liquid crystal
electrode
region
electrodes
crystal element
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
JP416090A
Other languages
Japanese (ja)
Inventor
Kenji Nakao
健次 中尾
Hisahide Wakita
尚英 脇田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP416090A priority Critical patent/JPH03209216A/en
Publication of JPH03209216A publication Critical patent/JPH03209216A/en
Pending legal-status Critical Current

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  • Liquid Crystal Display Device Control (AREA)

Abstract

PURPOSE:To display a half tone and to enable multilevel display without increasing the number of electrodes by providing a pattern having one electrode lack part at the electrode in each picture element at least and impressing a prescribed pulse voltage. CONSTITUTION:On an upper glass base 1, stripe-shaped transparent electrodes Y1-Y4 equipped with an electrode lack part 5a are formed and on a lower glass base 2, stripe-shaped transparent electrodes X1-X4 without the electrode lack part are formed. When a matrix driving waveform is impressed to such a liquid crystal panel, for the dark/bright state of the picture element, the area executing hutching is turned to the dark state. In such a way, since the state of the electrode lack part 5a provided in the picture element is controlled by the voltage to be impressed to the electrode, the multilevel display can be obtained with the same number of electrodes as normal ferroelectric liquid crystal. Thus, the stable multilevel display is obtained by a pair of picture element electrodes.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は強誘電性液晶を液晶層として持つ液晶素子とそ
の駆動法、及び表示装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a liquid crystal element having a ferroelectric liquid crystal as a liquid crystal layer, a driving method thereof, and a display device.

従来の技術 従来の強誘電性液晶素子としては、例えば第9図のよう
な構戒の液晶表示パネルがある。一方のガラス基板82
a上にカラーフィルター83と遮光層84を形威し、そ
の上を平滑化層85で覆った後、透明電極81を形威し
、,サらに配間脱86を塗布する。
2. Description of the Related Art As a conventional ferroelectric liquid crystal element, there is, for example, a structured liquid crystal display panel as shown in FIG. One glass substrate 82
After forming a color filter 83 and a light-shielding layer 84 on top a and covering it with a smoothing layer 85, a transparent electrode 81 is formed, and an interlayer 86 is applied on the surface.

他方のガラス基板82b上には透明電極81と配向膜8
6を付ける。これら一対の基板をスペーサ−88により
1.5μmから5μIn程度のある一定の間隔に対向さ
せ、その間に強誘電性液晶80を注入し、配向させる。
A transparent electrode 81 and an alignment film 8 are disposed on the other glass substrate 82b.
Add 6. These pair of substrates are opposed to each other by a spacer 88 at a certain distance of about 1.5 μm to 5 μIn, and a ferroelectric liquid crystal 80 is injected and aligned between them.

さらにカ゛ラス基板82a、R2bの外側に偏向し87
、検光子89を備える(例えば、村.1:.、石川他:
「高速マルチカラー強誘電性LCD,、第14回液晶討
論会予稿集、88頁から89貫)。薄膜化された強誘電
性液晶は基本的に第10図のような2つの状態が安定に
なる。第10図(a)、ら)は液晶分子の方向がほぼ揃
った状態で、このとき自発分極は基板法線上方及び下方
に向いている。直交させた偏光子102、103の間に
液晶セルを挟むと、第lO図(a)、(b)の一様な状
態を用いて、明暗を付けることができる。薄膜化した強
誘電性液晶パネルはこのような安定状態を持ち、かつ、
これらの状態間の遷移は印加電圧に応じて非常に急激に
起こり、印加電圧と透過光量の特性は急峻なしきい値特
性を示す。このため、薄膜トランジスタのような非線形
素子を設けなくても、単純なマトリックス構成の電極だ
けで大容量で高コントラストの表示を得ることができる
Furthermore, the glass substrates 82a and R2b are deflected to the outside and 87
, analyzer 89 (for example, Mura.1:., Ishikawa et al.:
"High-speed multicolor ferroelectric LCD," Proceedings of the 14th Liquid Crystal Conference, pp. 88-89).Thinned ferroelectric liquid crystals basically have two stable states as shown in Figure 10. In Fig. 10(a) and 10(a), the directions of the liquid crystal molecules are almost aligned, and the spontaneous polarization is directed above and below the normal line of the substrate. By sandwiching the liquid crystal cell, it is possible to create brightness and darkness using the uniform states shown in Figures 1O (a) and (b).A thin ferroelectric liquid crystal panel has such a stable state, and ,
Transitions between these states occur very rapidly depending on the applied voltage, and the characteristics of the applied voltage and amount of transmitted light exhibit steep threshold characteristics. Therefore, a high-capacity, high-contrast display can be obtained using only electrodes in a simple matrix configuration without providing a nonlinear element such as a thin film transistor.

しかしながら、強誘電性液晶は第10図のような限られ
た安定状態しかとれないので多階調を出し難い.また第
10図(a)と第10図6)が混在し、中間輝度を示す
状態が第10図(a)から第10図(b)の状態に変わ
る狭い電圧範囲で存在するが、液晶パネルに厚さ等の不
均一性が存在するため、実際に安定した中間調表示を実
現することは困難である。前記第10図(a)と第10
図(ロ)の混在状態を用いて中間調表示を行うために、
液晶層の厚さの異なる領域を各絵素内に設ける方式も提
案されているが(例えば、岩井、脇田他:r強誘電性液
晶の階調表示」、第13回液晶討論会講演予稿集、13
8頁から139真)、前記方式では液晶パネルの製造過
程が複雑に或るためにコストの上昇を招く。
However, ferroelectric liquid crystals can only take a limited stable state as shown in Figure 10, making it difficult to produce multiple gradations. In addition, Figure 10(a) and Figure 10(6) coexist, and a state showing intermediate brightness exists in a narrow voltage range where the state of Figure 10(a) changes to the state of Figure 10(b), but the liquid crystal panel Since there is non-uniformity in thickness, etc., it is difficult to actually achieve stable halftone display. Said FIG. 10(a) and FIG.
In order to display halftones using the mixed state shown in figure (b),
A system in which regions with different thicknesses of the liquid crystal layer are provided within each pixel has also been proposed (for example, Iwai, Wakita et al.: ``Gradation Display of Ferroelectric Liquid Crystals'', Proceedings of the 13th Liquid Crystal Symposium). , 13
(pp. 8-139), this method requires a complicated manufacturing process for the liquid crystal panel, leading to an increase in cost.

従って、通常は表面安定化強誘電性液晶は基本的には2
値表示で、複数の絵素や、複数回の走査によって階調を
出している(例えば、レルー他:1988インターナシ
ゴナルディスプレイリサーチコンファレンス予稿集、1
11頁(T.LEROtlX.F.BAUMB.et.
al.  : 1988 INTERNATIONAL
 DISPl.AY RESEACHCONFEREN
CE, pll1〜1133 )。
Therefore, surface-stabilized ferroelectric liquid crystals usually have basically two
In value display, gradation is produced by multiple picture elements or multiple scans (for example, Leroux et al.: Proceedings of the 1988 International Display Research Conference, 1).
Page 11 (T.LEROtlX.F.BAUMB.et.
al. : 1988 INTERNATIONAL
DISPl. AY RESEACH CONFEREN
CE, pll1-1133).

しかし、この方法は駆動回路数が増える等の課題が有る
。そこで、我々は特許願平1−2422号で絵素に挟ま
れた領域を絵素電極を介した電圧印加により少ない駆動
回路で安定に中間調を表示する方法を開示した。
However, this method has problems such as an increase in the number of drive circuits. Therefore, in patent application No. 1-2422, we have disclosed a method for stably displaying halftones with a small number of drive circuits by applying a voltage to a region between picture elements through picture element electrodes.

発明が解決しようとする課題 従来は、強誘電性液晶では階調を表示するために複数の
絵素を用いているが、このため電極数が増え、電極パタ
ーンが微細になり、駆動回路が増えるためコスト上昇と
なる.また絵素間隙部を用いる方法は駆動方法が複雑、
間隙部の形を自由に変えられないなどの課題がある. 課題を解決するための手段 上記課題を解決するために本発明の液晶素子は、対向面
に電極を有しマトリックス状の絵素を形成する基板間に
強誘電性液晶を挟持し、各絵素内の電極に少なくとも一
つ電極欠落部を有するパターンを持ち、所定のパルス電
圧を印加することにより、対向する電極に挟まれた第1
の領域と電極欠落部上の第2の領域の安定状態を切り替
えで、前記W41の領域と前記第2の領域の明暗の組合
せにより中間調を表示することができ、電極数を増やす
ことなく多階調表示ができる。
Problems to be Solved by the Invention Conventionally, ferroelectric liquid crystals use multiple picture elements to display gradations, but this increases the number of electrodes, makes the electrode pattern finer, and increases the number of drive circuits. Therefore, the cost will increase. In addition, the method using pixel gaps requires a complicated driving method.
There are issues such as not being able to freely change the shape of the gap. Means for Solving the Problems In order to solve the above problems, the liquid crystal element of the present invention has a ferroelectric liquid crystal sandwiched between substrates having electrodes on opposing surfaces and forming matrix-like picture elements, and each picture element By applying a predetermined pulse voltage, the first electrode sandwiched between the opposing electrodes has a pattern in which at least one electrode is missing.
By switching the stable state of the region W41 and the second region on the missing electrode part, it is possible to display halftones by the combination of brightness and darkness of the region W41 and the second region, and it is possible to display many gray scales without increasing the number of electrodes. Gradation display is possible.

作用 絵素内に微細な電極欠落部が存在する場合、上下とも電
極で挟まれた第1の領域と同様に前記電極欠落部上の第
2の領域も電界に応答し、第2の領域は第1の領域と同
様な安定状態をとる。第2の領域の液晶のしきい値電圧
は第1の領域のしきい4m電圧よりも高いが、十分な電
圧、パルス幅を印加することにより安定状態は切り替わ
る。強誘電性液晶の応答は概ね、電圧とパルス幅の積に
比例するが、簡単のために各絵素内に単一幅の電極欠落
部を1つ有する液晶パネルを想定し、パルス幅を固定し
たときの、第1の領域の液晶の安定状態が明から暗、暗
から明に切り替わるしきい値電圧をーvpci,vpb
、第2の領域の安定状態が明から暗、暗から明に切り替
わるときに電極に印加されている電圧を−Vsd、Vs
bとすると、Vsd>Vpd Vsb>Vpb の関係がある。前記第2の領域のしきい値電圧■sd,
Vsbは電極欠落部の幅の増加に伴い増加する。一Vs
d以下の電圧で第1の領域、第2の領域の双方を暗状態
にしたあと、選択期間の絵素へ印加する電圧をv1、v
2、v3として、V1≧Vs b>V2>Vpb>V3 の関係がある場合、印加電圧がv1の時は第1の領域、
第2の領域ともに明状態になり、V2の時は第1の領域
のみ明、第2の領域は暗となり、■3の時はどちらも暗
状態になる。従ってv2の時には中間輝度を1回の走査
で得ることができ、V2は、 Vsb>V2>Vpd となる電圧範囲を持つために液晶パネルに不均一がある
場合にも、安定した中間調表示が可能である。
When a minute electrode missing part exists in the active picture element, the second area above the electrode missing part also responds to the electric field in the same way as the first area sandwiched between the upper and lower electrodes, and the second area responds to the electric field. It assumes a stable state similar to the first region. Although the threshold voltage of the liquid crystal in the second region is higher than the threshold 4m voltage in the first region, the stable state can be switched by applying a sufficient voltage and pulse width. The response of a ferroelectric liquid crystal is roughly proportional to the product of voltage and pulse width, but for simplicity, we assume a liquid crystal panel with one single-width electrode missing part in each pixel and fix the pulse width. The threshold voltage at which the stable state of the liquid crystal in the first region switches from bright to dark and from dark to bright when
, the voltages applied to the electrodes when the stable state of the second region switches from bright to dark and from dark to bright are −Vsd, Vs
b, there is a relationship of Vsd>Vpd and Vsb>Vpb. The threshold voltage ■sd of the second region,
Vsb increases as the width of the electrode missing portion increases. One Vs
After darkening both the first region and the second region with a voltage equal to or lower than d, the voltages applied to the picture elements during the selection period are set to v1 and v.
2. As v3, if there is a relationship of V1≧Vs b>V2>Vpb>V3, when the applied voltage is v1, the first region,
Both the second areas are in a bright state; at V2, only the first area is bright and the second area is dark; at (3), both are in a dark state. Therefore, when using v2, intermediate brightness can be obtained in one scan, and since V2 has a voltage range of Vsb>V2>Vpd, stable halftone display can be achieved even if there is unevenness in the liquid crystal panel. It is possible.

中間輝度は絵素内に設ける電極欠落部の面積に依存し、
絵素内に設ける電極欠落部の面積を絵素面積の3分の1
にとることで等間隔の中間調が得られる。また幅の異な
る電極欠落部を絵素内にN個設けることで1回の走査で
N+2階調表示が可能であり、N+1回の走査で2”−
’itl!表示が可能である, また電極欠落部の幅が大きな場合は、■1と■3の値が
離れすぎるため、1回の走査では制御できないが、電極
欠落部上の第2の領域を切り替える走査と電極で挟まれ
た第1の領域を切り替える走査を分け、2回の走査で書
き込むことが実現できる。
The intermediate brightness depends on the area of the electrode missing part provided within the picture element,
The area of the electrode missing part provided within the picture element is one-third of the picture element area.
By setting it to , evenly spaced halftones can be obtained. In addition, by providing N electrode missing parts with different widths within a picture element, it is possible to display N+2 gradations in one scan, and 2"-2" in N+1 scans.
'itl! In addition, if the width of the electrode missing part is large, the values of ■1 and ■3 are too far apart, so it cannot be controlled with one scan, but a scan to switch the second area on the electrode missing part By dividing the scanning for switching the first region sandwiched between the electrodes and the first region between the electrodes, writing can be realized by two scannings.

実施例 以下本発明の一実施例を液晶素子とその駆動法について
、図面を参照しながら説明する。
EXAMPLE Hereinafter, an example of the present invention will be described with reference to the drawings regarding a liquid crystal element and its driving method.

第1図、第2図は本発明の一実施例の液晶素子の平面図
と断面図である.上部ガラス基板l上に電極欠落部5a
、5bを有するストライブ状の透明電極Y1〜Y4を、
下部ガラス基12には電極欠落部のないストライブ状の
透明電極X1〜X4を形威した.電極XI−X4、Y1
〜Y4のピッチは18μm,電極間間隙部は2μmとし
、上部ガラス基板1の電極Y1〜Y4に、長さ14μm
で幅2μm,4μmの2つの電極欠落部5を各絵素に有
するように電極群を構成した。この双方基板上にSiO
を基板法線から82度傾いた方向から蒸着し、配向81
113を形威している.この上下基板間にエステル系の
強誘電性液晶を封入し、強誘電性液晶層l4の厚さを2
.0μmとした。この液晶パネルに第3図のようなマト
リクス駆動波形を印加した場合、絵素の明暗の状態は第
1図に示したとおりであり、ハンチングを施した領域が
暗状態である.第4図、第5図は第1図の構或の液晶パ
ネルの光透過率を測定した特性図で、第6図のような電
圧を絵素に印加しており、パルス幅1ミリ秒で25ボル
トの交流パルスで全画面を暗状態にしてから、極性の順
序が逆の交流テストパルスを印加した後の安定した状態
の光透過率を測定している。第4図a.b,cはそれぞ
れ電圧を25ボルトに固定してテストパルスの幅τを変
えた時の、電極で挟まれた第1の領域、電極欠落部!(
5a)上の第2の領域、電極欠落部n(5b)上の第3
の領域の光透過率を測定した特性曲線で、それぞれ20
0μ秒、350μ秒、500μ秒で安定状態が切り替わ
っごいる。第5IiJa,b,cはτを500μ秒に固
定したときの第1の領域、第2の領域、第3の領域の特
性曲線で、それぞれのしきい値電圧は10ボルト、14
ポルト、22ポルトとなった。このように電極で挟まれ
た第1の領域、電極欠落部上の第2の頭域と第3の領域
は共に双安定性を示し、電極欠落部の幅が大きいほど、
しきい値パルス幅、しきい値電圧は増大することが分か
った。
1 and 2 are a plan view and a sectional view of a liquid crystal element according to an embodiment of the present invention. Electrode missing portion 5a on the upper glass substrate l
, 5b, strip-shaped transparent electrodes Y1 to Y4 have
The lower glass base 12 is provided with striped transparent electrodes X1 to X4 with no electrode missing parts. Electrodes XI-X4, Y1
~The pitch of Y4 is 18 μm, the gap between the electrodes is 2 μm, and the electrodes Y1 to Y4 of the upper glass substrate 1 have a length of 14 μm.
The electrode group was constructed so that each picture element had two electrode missing parts 5 with widths of 2 μm and 4 μm. SiO on both substrates
is deposited from a direction inclined at 82 degrees from the normal line of the substrate, with an orientation of 81
It resembles 113. Ester-based ferroelectric liquid crystal is sealed between the upper and lower substrates, and the thickness of the ferroelectric liquid crystal layer l4 is reduced to 2.
.. It was set to 0 μm. When a matrix driving waveform as shown in Fig. 3 is applied to this liquid crystal panel, the bright and dark states of the picture elements are as shown in Fig. 1, and the hunting area is in the dark state. Figures 4 and 5 are characteristic diagrams obtained by measuring the light transmittance of the liquid crystal panel with the structure shown in Figure 1.The voltage shown in Figure 6 was applied to the picture element, and the pulse width was 1 millisecond. After darkening the entire screen with a 25 volt alternating current pulse, the light transmittance in a stable state was measured after applying an alternating current test pulse with the reverse polarity order. Figure 4 a. b and c are the first region sandwiched between the electrodes, the electrode missing part, when the voltage is fixed at 25 volts and the test pulse width τ is varied! (
5a), the third region on the electrode missing part n(5b)
This is a characteristic curve that measures the light transmittance in the area of 20
The stable state changes at 0 μs, 350 μs, and 500 μs. 5IiJa, b, c are characteristic curves of the first region, second region, and third region when τ is fixed at 500 μs, and the respective threshold voltages are 10 volts and 14 volts.
Porto became 22 Porto. In this way, the first region sandwiched between the electrodes, the second head region and the third region above the electrode missing part both exhibit bistability, and the larger the width of the electrode missing part, the more
It was found that the threshold pulse width and threshold voltage increased.

前記しきい値特性を用い複数回の走査によって8階調表
示を行なった実施例を示す。液晶パネルに第3図のよう
な駆動波形を印加し、第1の領域、電極欠落部1(5a
)上の第2の領域、電極欠落部II(5b)上の第3の
領域の明暗状態を組み合わせて階調表示を行なった.第
3図でまず±25ボルト、1ミリ秒のリセットバルス3
0を印加して第1の領域、第2の領域、第3の領域を含
むパルス全面を暗状態にした後、第3の領域、第2の領
域、第1の領域をそれぞれしきい値パルス幅の長い部分
から順に31から33の3回の走査を行なって3つの部
分の明暗をそれぞれ独立に付け、その組合せで階調表示
ができた。例えば第3図の波形はAは第1図の行電極X
lへの印加電圧、Bは列電極Y3への印加電圧、Cは桧
素(Xi、Y3)への印加電圧であり、これにより第2
の領域のみを暗状態に第1の領域、第3の領域を明状態
にできる。
An example will be described in which 8-gradation display is performed by scanning a plurality of times using the threshold characteristic. A driving waveform as shown in Fig. 3 is applied to the liquid crystal panel, and the first area, the electrode missing part 1 (5a
), and the brightness and darkness of the second region on the electrode missing part II (5b) were combined to perform gradation display. In Figure 3, first reset pulse 3 of ±25 volts, 1 millisecond.
0 is applied to bring the entire pulse area including the first, second, and third regions into a dark state, and then a threshold pulse is applied to the third, second, and first regions, respectively. Scanning was performed three times from 31 to 33 in order from the widest part, and the brightness and darkness of the three parts were independently applied, and a gradation display was made by combining them. For example, in the waveform of FIG. 3, A is the row electrode X of FIG.
B is the voltage applied to column electrode Y3, C is the voltage applied to Xi (Xi, Y3), and this causes the second
It is possible to make only the region in the dark state and the first region and the third region in the bright state.

1回目の走査34ではパルス幅600μ秒であり、この
とき絵素に印加されるパルスの極性はリセットパルスと
逆転しているため第1の領域、第2の領域、第3の領域
はすべて明状態になる。これを1走査線づつ順次ずらし
ていくと、各絵素の電極欠落部n(5b)上の第3の領
域にデータを書き込むことができる。次に2回目の走査
35ではパルス幅400μ秒とし、第1の領域、第2の
領域を暗状態に変化させるが、第3の領域はしきい値電
圧が高いために以前の明状態を保持する。これにより電
極欠落部1(5a)上の第2の領域のデータを書き込む
ことができる。これを各行電極で順次走査させた後、3
回目の走査36ではパルス幅250μ秒で、第1の領域
のみを明状態に変化させ、第1の領域、第3の領域はし
きい値電圧が高いため、以前の状態を保持する.これに
より第1の領域のデータを書き込むことができる。これ
らの走査によって第lの領域、第2の領域、第3の領域
をそれぞれ独立にデータを書き込むことができた。
In the first scan 34, the pulse width is 600 μs, and the polarity of the pulse applied to the picture element is reversed from the reset pulse, so the first, second, and third regions are all bright. become a state. By sequentially shifting this one scanning line at a time, data can be written in the third region on the electrode missing portion n (5b) of each picture element. Next, in the second scan 35, the pulse width is 400 μs, and the first region and the second region are changed to a dark state, but the third region maintains its previous bright state because the threshold voltage is high. do. Thereby, data in the second region on the electrode missing portion 1 (5a) can be written. After sequentially scanning this with each row electrode, 3
In the second scan 36, only the first region is changed to a bright state with a pulse width of 250 μsec, and since the threshold voltage of the first region and the third region is high, the previous state is maintained. This allows data in the first area to be written. These scans made it possible to write data independently in the first area, second area, and third area.

次に1回の走査で4階調表示ができた第2の実施例を示
す.第1図で示されたような液晶パネルの電極(x1〜
X4、Y1〜Y4)のパターンを、電極ピッチ18μm
,it極間間隙部2μm、とし、下部ガラス基板(1)
上の電極に幅1μmの電極欠落部r (5a)、2um
の電極欠落部II(5b)の2つを有する強誘電性液晶
マトリクスバネルを用いた.第6図の駆動波形をパルス
幅250μ秒で印加し、パネル全体の光透過率特性を測
定すると第7図の特性図が得られ、対向する電極で挟ま
れた第1の領域、電極欠落部1 (5a)上の第2の領
域、電極欠落部II(5b)上の第3の領域それぞれの
透過光量を足した場合の透過率を縦軸に取っている。2
0ボルトで第lの領域が応答し、26ボルトで第2の領
域が応答し、ついで28ボルトで第3の領域が応答して
いる。従ってパルス$51 250μ秒、オン電圧29
ボルト、バイアス比1/4で駆動して、オン電圧29ボ
ルト、オフ電圧18ボルト、中間電圧125ボルト中間
電圧[27ボルトの選択電圧を印加すると1回の走査で
4階調の表示ができた。
Next, we will show a second example that can display four gradations in one scan. The electrodes of the liquid crystal panel (x1~
X4, Y1 to Y4) pattern with an electrode pitch of 18 μm.
, it is assumed that the gap between the electrodes is 2 μm, and the lower glass substrate (1)
Electrode missing part r (5a) with a width of 1 μm on the upper electrode, 2 μm
A ferroelectric liquid crystal matrix panel having two electrode missing parts II (5b) was used. When the drive waveform shown in Fig. 6 is applied with a pulse width of 250 μs and the light transmittance characteristics of the entire panel are measured, the characteristic diagram shown in Fig. 7 is obtained, and the first region sandwiched between opposing electrodes, the electrode missing part 1 (5a) and the third region on the electrode missing portion II (5b) are added together, and the transmittance is plotted on the vertical axis. 2
At 0 volts the first region responds, at 26 volts the second region responds, and then at 28 volts the third region responds. Therefore pulse $51 250μsec, on voltage 29
volts, bias ratio 1/4, on voltage 29 volts, off voltage 18 volts, intermediate voltage 125 volts [If a selection voltage of 27 volts was applied, 4 gray scales could be displayed in one scan. .

中間電圧lでは第1の領域のみが明状態になり、中間電
圧■では第1の領域と第2の領域のみが明状態になり、
オン電圧ですべての領域が明状態になる。
At an intermediate voltage l, only the first region becomes a bright state, and at an intermediate voltage ■, only the first region and the second region become a bright state,
All areas become bright at on-voltage.

以上のように本発明の液晶素子は、絵素内に設けた電極
欠落部の状態を電極に印加する電圧によって制御するこ
とにより、従来の強誘電性液晶と同じ!極数で多liI
調表示を実現する。
As described above, the liquid crystal element of the present invention is the same as the conventional ferroelectric liquid crystal by controlling the state of the electrode missing part provided in the picture element by the voltage applied to the electrode! Large number of poles
Achieve gradation display.

さらに、本発明の液晶素子とその駆動法を用いて従来に
ない高精細大容量の表示装置が実現できる。前記表示装
置のブロック図を第8図に示す。
Furthermore, by using the liquid crystal element of the present invention and its driving method, an unprecedented high-definition, large-capacity display device can be realized. A block diagram of the display device is shown in FIG.

また特に絵素ピンチが数十μm以下のパターンの場合に
は、スクリーン上に拡大投射することにより大型で高精
細大容量で、かつ、高コントラストで、多階調の表示装
置を構或できる。
In particular, in the case of a pattern in which the pixel pinch is several tens of micrometers or less, by enlarging and projecting the image onto a screen, a large, high-definition, large-capacity, high-contrast, multi-gradation display device can be constructed.

発明の効果 本発明の液晶素子は、所定の電圧波形を絵素電極に印加
して、絵素内に設けた電極欠落部の強誘電性液晶分子を
電界に応答させ、安定状態を切り替えることにより、1
対の絵素電極で安定した多階調の表示を行なうことがで
きる。
Effects of the Invention The liquid crystal element of the present invention applies a predetermined voltage waveform to the picture element electrode, causes the ferroelectric liquid crystal molecules in the electrode missing part provided in the picture element to respond to the electric field, and switches the stable state. ,1
Stable multi-gradation display can be performed using a pair of picture element electrodes.

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

第1図は、第2図は本発明の一実施例の液晶素子の平面
図と、断面図、第3図は本発明の液晶素子の駆動法の波
形図、第4図、第5図は本発明の液晶素子の特性図、第
6図は特性測定時の印加電圧の波形図、第7図は第2の
実施例の本発明の液晶素子の特性図、第8図は本発明の
液晶表示装置のブロック図、第9図は従来例の強誘電性
液晶パネルの構成図、第lO図は強誘電性液晶分子の安
定状態の模式図である。 l・・・・・・上基板、2・・・・・・下基板、3・・
・・・・列電極群、4・・・・・・行電極群、5・・・
・・・電極欠落部、13・・・・・・配向膜、l4・・
・・・・強誘電性液晶層、A・・・・・・行電極X1へ
の印加電圧、B・・・・・・列電極Y3への印加電圧、
C・・・・・・絵素(Xi、Y3)への印加電圧、30
・・・・・・リセットパルス、31・・・・・・第1走
査、32・・・・・・第2走査、33・・・・・・第3
走査.
FIG. 1 is a plan view and a cross-sectional view of a liquid crystal element according to an embodiment of the present invention, FIG. 3 is a waveform diagram of a driving method for a liquid crystal element according to the present invention, and FIGS. A characteristic diagram of the liquid crystal element of the present invention, FIG. 6 is a waveform diagram of the applied voltage during characteristic measurement, FIG. 7 is a characteristic diagram of the liquid crystal element of the present invention of the second embodiment, and FIG. FIG. 9 is a block diagram of a display device, FIG. 9 is a configuration diagram of a conventional ferroelectric liquid crystal panel, and FIG. 10 is a schematic diagram of a stable state of ferroelectric liquid crystal molecules. l...upper board, 2...lower board, 3...
...Column electrode group, 4... Row electrode group, 5...
...Electrode missing part, 13...Alignment film, l4...
... Ferroelectric liquid crystal layer, A... Voltage applied to row electrode X1, B... Voltage applied to column electrode Y3,
C... Voltage applied to picture element (Xi, Y3), 30
...Reset pulse, 31...First scan, 32...Second scan, 33...Third
scanning.

Claims (9)

【特許請求の範囲】[Claims] (1)対向面に電極を有し、マトリクス状の絵素を形成
する基板間に強誘電性液晶を挟持し、各絵素内の電極に
少なくとも1つの電極欠落部を有するパターンを持つこ
とにより、各絵素内の対向する電極で挟まれた第1の領
域と電極欠落部上の第2の領域の安定状態を切り替え、
前記第1の領域と前記第2の領域の明暗の組合せにより
中間調を表示することを特徴とする液晶素子。
(1) By sandwiching a ferroelectric liquid crystal between substrates that have electrodes on opposing surfaces and forming matrix-like picture elements, and having a pattern in which the electrodes in each picture element have at least one electrode missing part. , switching the stable state of a first region sandwiched between opposing electrodes in each picture element and a second region above the electrode missing part,
A liquid crystal device characterized in that an intermediate tone is displayed by a combination of brightness and darkness of the first region and the second region.
(2)1回の走査で絵素内の電極部、電極欠落部の明暗
を制御し多階調を表示できる請求項(1)記載の液晶素
子。
(2) The liquid crystal element according to claim (1), wherein the liquid crystal element can display multiple gradations by controlling the brightness of the electrode portions and electrode missing portions within the picture element in one scan.
(3)第1の領域、第2の領域が共に急峻な応答しきい
値特性を示し、前記第1、第2の二つの領域のしきい値
電圧が異なっており、安定な中間調を表示されることを
特徴とする請求項(1)記載の液晶素子。
(3) Both the first region and the second region exhibit steep response threshold characteristics, the threshold voltages of the first and second regions are different, and stable halftones are displayed. The liquid crystal element according to claim 1, characterized in that:
(4)前記第1の領域と前記第2の領域の面積比が2:
1である請求項(1)記載の液晶素子。
(4) The area ratio of the first region and the second region is 2:
1. The liquid crystal element according to claim 1, which is
(5)面積の異なる複数の電極欠落部を有する請求項(
1)記載の液晶素子。
(5) Claim having a plurality of electrode missing parts with different areas (
1) The liquid crystal element described above.
(6)対向面に電極を有しマトリックス状の絵素を形成
する基板間に強誘電性液晶を挟持する液晶素子の駆動法
において、前記電極に選択走査電圧を印加し、対向面の
電極には前記選択走査電圧を印加した電極及び電極欠落
部で構成される絵素の画像データに対応する信号電圧を
印加することにより、対向する電極に挟まれた第1の領
域及び電極欠落部上の第2の領域の安定状態を制御する
ことを特徴とする液晶素子の駆動法。
(6) In a method for driving a liquid crystal element in which a ferroelectric liquid crystal is sandwiched between substrates having electrodes on opposing surfaces and forming a matrix of picture elements, a selective scanning voltage is applied to the electrodes, and a selective scanning voltage is applied to the electrodes on the opposing surfaces. By applying a signal voltage corresponding to the image data of the picture element consisting of the electrode to which the selective scanning voltage is applied and the electrode missing part, the first area sandwiched between the opposing electrodes and the electrode missing part are A method for driving a liquid crystal element, characterized by controlling a stable state of a second region.
(7)1回の走査で絵素内の電極部、電極欠落部の明暗
を制御し多階調を表示できる請求項(5)記載の液晶素
子の駆動法。
(7) The method for driving a liquid crystal element according to claim (5), wherein the brightness and darkness of the electrode portion and the electrode missing portion within the picture element can be controlled in one scan to display multiple gradations.
(8)電極欠落部の安定状態を制御する第1の走査の後
に電極部の安定状態を制御する第2の走査を行う請求項
(5)記載の液晶素子の駆動法。
(8) The method for driving a liquid crystal element according to claim 5, wherein a second scan for controlling the stable state of the electrode portion is performed after the first scan for controlling the stable state of the electrode missing portion.
(9)対向面に電極を有し、マトリックス状の絵素を形
成する基板間に強誘電性液晶を挟持し、各絵素内の電極
に少なくとも1つの電極欠落部を有するパターンを持つ
液晶表示素子を用い、前記電極に選択走査電圧を印加し
、対向面の電極には前記選択走査電圧を印加した電極及
び電極欠落部で構成される絵素の画像データに対応する
信号電圧を印加することにより、対抗する電極に挟まれ
た第1の領域及び電極欠落部上の第2の領域の安定状態
を制御することを特徴とする液晶素子の駆動法を実現す
る回路からなる液晶表示装置。
(9) A liquid crystal display having a pattern in which a ferroelectric liquid crystal is sandwiched between substrates that have electrodes on opposing surfaces and form matrix-like picture elements, and each picture element has at least one electrode missing part. applying a selective scanning voltage to the electrode using an element, and applying a signal voltage corresponding to image data of a pixel consisting of the electrode to which the selective scanning voltage was applied and the electrode missing portion to the electrode on the opposing surface; 1. A liquid crystal display device comprising a circuit for realizing a method for driving a liquid crystal element, characterized in that the stable state of a first region sandwiched between opposing electrodes and a second region on an electrode missing portion is controlled by:
JP416090A 1990-01-11 1990-01-11 Liquid crystal element, driving method for the same and liquid crystal display device Pending JPH03209216A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP416090A JPH03209216A (en) 1990-01-11 1990-01-11 Liquid crystal element, driving method for the same and liquid crystal display device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP416090A JPH03209216A (en) 1990-01-11 1990-01-11 Liquid crystal element, driving method for the same and liquid crystal display device

Publications (1)

Publication Number Publication Date
JPH03209216A true JPH03209216A (en) 1991-09-12

Family

ID=11576992

Family Applications (1)

Application Number Title Priority Date Filing Date
JP416090A Pending JPH03209216A (en) 1990-01-11 1990-01-11 Liquid crystal element, driving method for the same and liquid crystal display device

Country Status (1)

Country Link
JP (1) JPH03209216A (en)

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