JP2731916B2 - Ferroelectric liquid crystal cell - Google Patents
Ferroelectric liquid crystal cellInfo
- Publication number
- JP2731916B2 JP2731916B2 JP63218526A JP21852688A JP2731916B2 JP 2731916 B2 JP2731916 B2 JP 2731916B2 JP 63218526 A JP63218526 A JP 63218526A JP 21852688 A JP21852688 A JP 21852688A JP 2731916 B2 JP2731916 B2 JP 2731916B2
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- liquid crystal
- ferroelectric liquid
- metal wiring
- crystal cell
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Description
【発明の詳細な説明】 ［産業上の利用分野］ 本発明は、ディスプレイ等に応用される強誘電性液晶
セル、特にA.C.スタビライズ方式を利用した強誘電性液
晶セルに関し、詳しくは、液晶の配向を制御する電極に
所定の抵抗分布を形成することにより温度分布を均一化
し、むらのない絵出しを可能とした強誘電性液晶セルに
関する。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a ferroelectric liquid crystal cell applied to a display or the like, and more particularly to a ferroelectric liquid crystal cell using an AC stabilization method. The present invention relates to a ferroelectric liquid crystal cell which has a uniform temperature distribution by forming a predetermined resistance distribution on an electrode for controlling the liquid crystal, thereby enabling uniform drawing.
［従来の技術］ 従来、液晶分子の誘電異方性Δεが負である液晶はA.
C.電界の印加時に見かけのチルト角を増加させるという
現象を利用した、A.C.スタビライズ方式による強誘電性
液晶セルが提案されている。[Prior art] Conventionally, a liquid crystal in which the dielectric anisotropy Δε of liquid crystal molecules is negative is A.
C. A ferroelectric liquid crystal cell using an AC stabilization method, which utilizes a phenomenon that an apparent tilt angle is increased when an electric field is applied, has been proposed.
このように、A.C.スタビライズ方式による強誘電性セ
ルは、駆動時の見かけのチルト角が非駆動時の見かけの
チルト角より大きいことを特徴としており、分子が大き
くねじれたスプレイ（splay）状態の配向となることを
利用した駆動方式（スプレイ駆動方式）のものに比べ
て、表示状態での明るさが２〜３倍程度増加するという
利点を有する。As described above, the AC stabilizing ferroelectric cell is characterized in that the apparent tilt angle when driven is larger than the apparent tilt angle when not driven, and the splay state of molecules is greatly twisted. There is an advantage that the brightness in the display state is increased by about two to three times as compared with the driving method (spray driving method) utilizing the above.
［発明が解決しようとする課題］ しかしながら、A.C.スタビライズ方式による強誘電性
液晶（FLC）セルに使用できる強誘電性液晶材料の誘電
率は、一般に大きい。このため、マトリクス駆動におい
て、A.C.スタビライズ方式のFLCセルは、電極とFLCで形
成されるコンデンサへの充電電流が増加するために、発
熱量がスプレイ駆動方式のFLCセルに比べて著しく増
加、しかもマトリクス回路構造に関係してセル内にかな
り不均一な温度分布をつくり出す。したがって、通常の
環境下で75cm2程度のA.C.スタビライズ用のFLCセルの絵
出しを試みる場合、不均一な温度分布のために５〜10分
程度で均一な全体の絵出しが不可能となってしまうとい
う問題点があった。[Problems to be Solved by the Invention] However, the dielectric constant of a ferroelectric liquid crystal material that can be used for a ferroelectric liquid crystal (FLC) cell using an AC stabilization method is generally large. For this reason, in matrix driving, the AC stabilization type FLC cell generates a large amount of heat compared to the spray driving type FLC cell because the charging current to the capacitor formed by the electrode and the FLC increases. It creates a rather non-uniform temperature distribution in the cell in relation to the circuit structure. Therefore, when attempting to paint a FLC cell for AC stabilization of about 75 cm 2 under a normal environment, it is impossible to paint a uniform whole in about 5 to 10 minutes due to uneven temperature distribution. There was a problem that it would.
本発明の目的は、このような従来技術の問題点に鑑
み、強誘電性液晶セルにおいて、セル内の温度分布を均
一化し、むらのない絵出しを長時間継続できるようにす
ることにある。SUMMARY OF THE INVENTION An object of the present invention is to provide a ferroelectric liquid crystal cell having a uniform temperature distribution in a ferroelectric liquid crystal cell so that uniform image display can be continued for a long time.
［課題を解決するための手段］ 上記目的を達成するため本発明では、ストライプ状の
電極を形成した基板を対向配置し、その間に強誘電性液
晶を挟持し、該電極を介して該強電性液晶の配向を制御
する強誘電性液晶セルにおいて、該電極の長さ方向に所
定の抵抗分布を形成するようにしている。[Means for Solving the Problems] In order to achieve the above object, in the present invention, a substrate on which stripe-shaped electrodes are formed is opposed to each other, a ferroelectric liquid crystal is interposed therebetween, and the ferroelectric liquid crystal is interposed between the substrates. In a ferroelectric liquid crystal cell for controlling the alignment of liquid crystal, a predetermined resistance distribution is formed in the length direction of the electrode.
前記所定の抵抗分布は、前記電極を強誘電性液晶セル
の表示部において該電極の長さ方向に抵抗値におりほぼ
ｎ等分の領域に分割し、該電極の駆動源から遠い側から
Ｓ番目（Ｓ＝1,2…ｎ）の領域の抵抗値RSを とするような抵抗分布であることが特に好ましい。この
ような抵抗分布は、例えば電極の断面積を順次小さくし
あるいは電極に順次幅が狭くなる複数間隔部分を設ける
ことにより形成される。The predetermined resistance distribution is such that the electrode has a resistance value in the length direction of the electrode in the display portion of the ferroelectric liquid crystal cell and is divided into substantially n equal regions, and S is divided from a side far from the drive source of the electrode. The resistance value R S of the region (S = 1, 2,... N) It is particularly preferable that the resistance distribution is as follows. Such a resistance distribution is formed by, for example, sequentially reducing the cross-sectional area of the electrode or providing the electrode with a plurality of intervals where the width is gradually reduced.
電極は、通常、抵抗の小さい金属配線部分と抵抗の非
常に大きい透明電極部分とを備えており、金属部分のみ
を上記のように構成することにより、上記の抵抗分布が
形成される。The electrode usually includes a metal wiring portion having a low resistance and a transparent electrode portion having a very high resistance, and the above-described resistance distribution is formed by configuring only the metal portion as described above.
［作用］ この構成において、駆動時には、電極に形成された抵
抗分布によってセル内の発熱分布に所定の変化が与えら
れ、これによってセル内の温度分布は一様化される。し
たがって、長時間であっても均質な絵出しが継続され
る。電極を流れる電流は駆動源（＝電流源）から遠ざか
るにつれて一般に小さくなるから、単位長さあたりの抵
抗値を電流源から遠ざかる方向に沿って大きくなるよう
に分布させることにより、発熱分布を均一化させること
ができる。[Operation] In this configuration, at the time of driving, a predetermined change is given to the heat generation distribution in the cell due to the resistance distribution formed on the electrode, whereby the temperature distribution in the cell is made uniform. Therefore, uniform drawing is continued even for a long time. Since the current flowing through the electrode generally decreases as the distance from the drive source (= current source) increases, the resistance value per unit length is distributed so as to increase in the direction away from the current source, so that the heat generation distribution is uniform. Can be done.
［実施例］ 以下、図面を用いて本発明の実施例を説明する。Embodiment An embodiment of the present invention will be described below with reference to the drawings.
実施例１ 第１図は本発明の第１の実施例に係る強誘電性液晶セ
ルの概念図である。この液晶セルは同図に示すように、
セグメント側透明電極１および配向膜２が形成されたセ
グメント側基板３、ならびにこれに対向して配置されコ
モン側透明電極４および配向膜２が形成されたコモン側
基板５を備え、セグメント側基板３とコモン側基板５と
の間に強誘電性液晶６を挟持している。Embodiment 1 FIG. 1 is a conceptual diagram of a ferroelectric liquid crystal cell according to a first embodiment of the present invention. This liquid crystal cell, as shown in FIG.
A segment-side substrate 3 having a segment-side transparent electrode 1 and an alignment film 2 formed thereon, and a common-side substrate 5 disposed opposite thereto and having a common-side transparent electrode 4 and an alignment film 2 formed thereon. A ferroelectric liquid crystal 6 is interposed between the ferroelectric liquid crystal 6 and the common-side substrate 5.
セグメント側透明電極１には所定の抵抗分布を有する
セグメント側金属配線７が、コモン側電極４には、コモ
ン側金属配線８が接続され、これらを介して駆動用の電
流がセグメントI.C.9およびコモンI.C.10から供給され
る。金属配線７とセグメント側透明電極１とでセグメン
ト電極11を構成している。The segment-side transparent electrode 1 is connected with a segment-side metal wiring 7 having a predetermined resistance distribution, and the common-side electrode 4 is connected with a common-side metal wiring 8, through which driving current is supplied to the segment IC 9 and the common IC 10. Supplied from The metal wiring 7 and the segment-side transparent electrode 1 constitute a segment electrode 11.
セグメント電極11とセグメント側の配向膜２との間、
およびコモン側透明電極４とコモン側の配向膜２との間
は、それぞれ透明絶縁膜12によって適宜絶縁されてい
る。Between the segment electrode 11 and the alignment film 2 on the segment side,
In addition, the common side transparent electrode 4 and the common side alignment film 2 are appropriately insulated by a transparent insulating film 12, respectively.
この構成において、電源投入後の駆動時には、セグメ
ント電極11はセル内の温度分布を均一化する作用を有
し、これによってA.C.スタビライズ状態での均一な絵出
しが長時間可能となる。In this configuration, at the time of driving after the power is turned on, the segment electrode 11 has a function of making the temperature distribution in the cell uniform, thereby enabling uniform drawing in the AC stabilized state for a long time.
第２図は所定の抵抗分布を有するセグメント電極11の
特徴を示す説明図である。セグメント電極11とセグメン
トI.C.9との間は接続部13により接続されている。ここ
では特に、セグメント電極11の表示部を適当にｎ等分
し、セグメントI.C.9から遠い側からC1…CS…Cnのよう
に各々の領域に番号を付したとすれば、Ｓ番目（Ｓ＝1,
2…ｎ）の領域の抵抗値RSを として、抵抗分布を形成することを特徴としている。す
なわち、より具体的には、（金属配線部分の抵抗）≪
（透明電極部分の抵抗）であることに注目し、特にセグ
メント側の金属配線７を適当にｎ等分し、セグメントI.
C.9から遠い側からC1…CS…Cnのように各々の領域に番
号を付したとすれば、Ｓ番目（Ｓ＝1,2…ｎ）の領域の
金属配線７の厚みdSを とすることによって としている。このように、金属配線部で抵抗を制御する
ことの利点は、抵抗制御が容易で生産工程が単純化でき
ることにある。FIG. 2 is an explanatory diagram showing characteristics of the segment electrode 11 having a predetermined resistance distribution. The connection section 13 connects between the segment electrode 11 and the segment IC 9. Here, in particular, a display of segment electrodes 11 appropriately divided into n equal parts, from the side far from the segment IC 9 C 1 ... and denoted by C S ... number to each region as C n, S-th ( S = 1,
The resistance value R S region of 2 ... n) Is characterized by forming a resistance distribution. That is, more specifically, (resistance of the metal wiring portion) ≪
(The resistance of the transparent electrode portion), and particularly, the metal wiring 7 on the segment side is appropriately divided into n equal parts.
Assuming that the respective regions are numbered as C 1 ... C S ... C n from the side farther from C.9, the thickness d of the metal wiring 7 in the S-th (S = 1, 2,. S By doing And The advantage of controlling the resistance in the metal wiring portion is that the resistance control is easy and the production process can be simplified.
第３図は、上述した金属配線７の厚みの変化によっ
て、抵抗分布を有する電極が形成されたFLCセルを模式
的に示した図である。FIG. 3 is a diagram schematically showing an FLC cell in which an electrode having a resistance distribution is formed by changing the thickness of the metal wiring 7 described above.
いま、上述のｎ分割領域に対応する抵抗分布をR1…RS
…Rnで表わし、これらで消費される電力について、第３
図（ｃ）のような近似的な等価回路によって考察する。
ここで、i1…iS…inは各々の領域における、電極とFLC
で形成されるコンデンサへの充電電流であり、近似的に
iS＝iO（＝一定）（ただし、Ｓ＝1,2…ｎ）とおける。
したがって、抵抗RSに流れる電流ISは、 となる。Now, the resistance distribution corresponding to n divided areas above R 1 ... R S
... expressed in R n, the power consumed by these third
Consider an approximate equivalent circuit as shown in FIG.
Here, i 1 ... i S ... i n is in each region, the electrode and the FLC
Is the charging current to the capacitor formed by
i S = i O (= constant) (where S = 1, 2,... n).
Accordingly, the current I S flowing through the resistor R S is Becomes
したがって、Ｓ番目の領域の抵抗RSで消費される電力
PSは、 の如く、セル内で一定となることがわかる。すなわち、
上述した抵抗分布によって、セル内の消費電力が均一化
され、セル内の温度分布も均一化されることがわかる。Therefore, the power consumed by the resistor R S in the Sth region
P S It can be seen that it becomes constant in the cell as shown in FIG. That is,
It can be seen that the above-described resistance distribution makes the power consumption in the cell uniform and the temperature distribution in the cell also uniform.
一方、同じく第３図（ｃ）より、抵抗分布を形成せ
ず、RS＝RO（＝一定）とした場合は、消費電力PS′は PS＝RS・IS 2＝R0（SiO）2 ＝s2ROiO 2（≠一定） となって、セル内に大きな温度分布を形成することがわ
かる。On the other hand, similarly from FIG. 3 (c), when the resistance distribution is not formed and R S = R O (= constant), the power consumption P S ′ is P S = R S · I S 2 = R 0 (Si 2 O 3 ) 2 = s 2 R O i O 2 (≠ constant), indicating that a large temperature distribution is formed in the cell.
以上の説明において、特に、セグメント電極側に抵抗
分布を形成した場合について述べたが、本発明の抵抗分
布はセグメント側に限定されるものではない。In the above description, particularly, the case where the resistance distribution is formed on the segment electrode side has been described, but the resistance distribution of the present invention is not limited to the segment side.
実施例２ 第４図は、本発明の第２の実施例に係る強誘電液晶セ
ルを示す説明図である。ここでは、特にセグメント側の
金属配線７を適当にｎ分割し、セグメントI.C.9から遠
い側からC1…CS…Cnのように各々の領域に番号を付すと
すれば、Ｓ番目（Ｓ＝1,2…ｎ）の領域の金属配線７の
幅WSを とすることによって上述と同様に、 とすることを特徴としている。これにより、実施例１と
同様に、温度分布が均一化され長時間の絵出しが可能と
なる。また、抵抗分布が容易に形成できる利点があり、
大量生産に適する。なお、第４図中14は、絶縁性遮光マ
スクである。Embodiment 2 FIG. 4 is an explanatory view showing a ferroelectric liquid crystal cell according to a second embodiment of the present invention. Here, in particular, if the metal wiring 7 on the segment side is appropriately divided into n and each region is numbered from the side far from the segment IC 9 as C 1 ... C S. The width W S of the metal wiring 7 in the region of 1, 2,. As described above, It is characterized by the following. As a result, as in the first embodiment, the temperature distribution is made uniform, and a long-time image can be displayed. In addition, there is an advantage that the resistance distribution can be easily formed,
Suitable for mass production. In FIG. 4, reference numeral 14 denotes an insulating light-shielding mask.
実施例３ 第５図は、本発明の第３の実施例に係る強誘電液晶セ
ルを示す説明図である。ここでは、特に、セグメント側
の金属配線７を適当にｎ分割し、セグメントI.C.9から
遠い側からC1…CS…Cnのように各々の領域に番号を付し
たとすれば、Ｓ番目（Ｓ＝1,2…ｎ）の領域の金属配線
部に金属配線のない部分（間隙）15を１つまたは複数個
配置し、Ｓ番目の間隙のギャップ幅gSを とすることによって とすることを特徴としている。Embodiment 3 FIG. 5 is an explanatory view showing a ferroelectric liquid crystal cell according to a third embodiment of the present invention. Here, in particular, if it is assumed that the metal wiring 7 on the segment side is appropriately divided into n and each region is numbered as C 1 ... C S. One or a plurality of portions (gaps) 15 having no metal wiring are arranged in the metal wiring portion in the region of S = 1, 2,... N), and the gap width g S of the S-th gap is determined. By doing It is characterized by the following.
実施例４ 第６図は本発明の第４の実施例に係る強誘電性液晶セ
ルを示す模式図である。ここでは、特に、コモン側電極
あるいはセグメント側電極あるいはその両方に全体的に
R1＜R2となる２つの異なる抵抗値領域を配置し、セグメ
ントI.C.9およびコモンI.C.10から遠い側の領域が、高
い側の抵抗値R2となるようにすることを特徴としてい
る。Embodiment 4 FIG. 6 is a schematic view showing a ferroelectric liquid crystal cell according to a fourth embodiment of the present invention. Here, in particular, the common-side electrode and / or the segment-side electrode
Two different resistance value regions satisfying R 1 <R 2 are arranged so that a region farther from the segment IC 9 and the common IC 10 has a higher resistance value R 2 .
従来、温度分布は、２つのドライバ用I.C.9,10から遠
い側の端が低温側となり、２つのドライバ用I.C.9,10か
ら近い側の端が高温側となっていたが、本実施例によれ
ば、従来の低温側近くの消費電力が増加することと、熱
の拡散作用とによってセル内の温度分布が均一化され
る。Conventionally, the temperature distribution is such that the end farther from the two driver ICs 9 and 10 has a lower temperature side and the end closer to the two driver ICs 9 and 10 has a higher temperature side. In addition, the conventional power consumption near the low temperature side increases, and the temperature distribution in the cell is made uniform by the heat diffusion action.
［発明の効果］ 以上説明したように本発明によれば、強誘電性液晶セ
ルにおいて、電極に所定の抵抗分布を形成するようにし
たため、セル内の温度分布の変化が抑制され、均一な絵
出しを長時間継続することができる。[Effects of the Invention] As described above, according to the present invention, in the ferroelectric liquid crystal cell, a predetermined resistance distribution is formed on the electrode. Dispensing can be continued for a long time.
第１図は、本発明の第１の実施例に係る強誘電性液晶セ
ルの概念図、 第２図は、第１図の装置のセグメント電極の特徴を示す
説明図、 第３図（ａ）〜（ｃ）は、第１図の装置を模式的に示し
てその原理を考察するための説明図、 第４図は、本発明の第２の実施例に係る強誘電性液晶セ
ルを示す説明図、 第５図は、本発明の第３の実施例に係る強誘電性液晶セ
ルを示す説明図、そして 第６図は、本発明の第４の実施例に係る強誘電性液晶セ
ルを示す模式図、 1:セグメント側基板、2:配向膜、3:セグメント側基板、
4:コモン側透明電極、5:コモン側基板、6:強誘電性液
晶、7:セグメント側金属配線、8:コモン側金属配線、9:
セグメント側I.C.、10:コモン側I.C.、11:抵抗分布を有
するセグメント電極、12:透明絶縁膜、13:接続部、14:
絶縁性遮光マスク、15:金属配線のない部分。FIG. 1 is a conceptual view of a ferroelectric liquid crystal cell according to a first embodiment of the present invention, FIG. 2 is an explanatory view showing the characteristics of the segment electrodes of the device of FIG. 1, and FIG. 4 (c) are explanatory diagrams for schematically illustrating the device of FIG. 1 and considering the principle thereof, and FIG. 4 is a diagram illustrating a ferroelectric liquid crystal cell according to a second embodiment of the present invention. FIG. 5, FIG. 5 is an explanatory view showing a ferroelectric liquid crystal cell according to a third embodiment of the present invention, and FIG. 6 is a view showing a ferroelectric liquid crystal cell according to a fourth embodiment of the present invention. Schematic diagram, 1: segment side substrate, 2: alignment film, 3: segment side substrate,
4: Transparent common side electrode, 5: Common side substrate, 6: Ferroelectric liquid crystal, 7: Segment side metal wiring, 8: Common side metal wiring, 9:
Segment side IC, 10: Common side IC, 11: Segment electrode with resistance distribution, 12: Transparent insulating film, 13: Connection, 14:
Insulating light-shielding mask, 15: Part without metal wiring.
Claims (9)
配置し、その間に強誘電性液晶を挟持し、該電極を介し
て該強電性液晶の配向を制御する強誘電性液晶セルにお
いて、該電極が該強誘電性液晶セルの表示部において該
電極の長さ方向に抵抗値によりほぼｎ等分の領域に分割
され、該電極の駆動源から遠い側からＳ番目（Ｓ＝1,2
…ｎ）の領域の抵抗値RSが であることを特徴とする強誘電性液晶セル。1. A ferroelectric liquid crystal cell in which a substrate on which stripe-shaped electrodes are formed is opposed to each other, a ferroelectric liquid crystal is interposed therebetween, and the orientation of the ferroelectric liquid crystal is controlled via the electrodes. The electrode is divided into substantially n equal regions in the display portion of the ferroelectric liquid crystal cell in the length direction of the electrode by a resistance value, and the S-th region (S = 1, 2) from the side farther from the driving source of the electrode.
The resistance value R S of the area of the ... n) A ferroelectric liquid crystal cell, characterized in that:
該金属配線部の厚さは駆動源から遠ざかるにつれて薄く
なる、請求項１記載の強誘電性液晶セル。2. The method according to claim 1, wherein the electrode includes a transparent electrode and a metal wiring part.
2. The ferroelectric liquid crystal cell according to claim 1, wherein the thickness of the metal wiring portion decreases as the distance from the driving source increases.
該金属配線部は厚みによりほぼｎ等分の領域に分割され
ており、前記電極に接続する駆動源から遠い側からＳ番
目（Ｓ＝1,2…ｎ）の領域の金属配線部の厚みdSが である、請求項１記載の強誘電性液晶セル。3. The device according to claim 1, wherein the electrode comprises a transparent electrode and a metal wiring part.
The metal wiring portion is divided into approximately n equal regions by thickness, and the thickness d of the metal wiring portion in the S-th (S = 1, 2,... N) region from the side far from the drive source connected to the electrode S is The ferroelectric liquid crystal cell according to claim 1, wherein
該金属配線部の幅が駆動源から遠ざかるにつれて小さく
なる、請求項１記載の強誘電性液晶セル。4. The electrode comprises a transparent electrode and a metal wiring portion,
2. The ferroelectric liquid crystal cell according to claim 1, wherein the width of the metal wiring portion decreases as the distance from the driving source increases.
え、該金属配線部は幅によりほぼｎ等分の領域に分割さ
れており、前記電極に接続する駆動源から遠い側からＳ
番目（Ｓ＝1,2…ｎ）の領域の金属配線部の幅WSが である、請求項１記載の強誘電性液晶セル。5. An electrode comprising a transparent electrode and a metal wiring portion, wherein the metal wiring portion is divided into a region substantially equal to n by width, and the metal wiring portion is formed from a side far from a driving source connected to the electrode.
The width W S of the metal wiring portion of the region (S = 1, 2,... N) is The ferroelectric liquid crystal cell according to claim 1, wherein
該金属配線部は駆動源から遠ざかるにつれて広くなる複
数のギャップを有する、請求項１記載の強誘電性液晶セ
ル。6. An electrode comprising a transparent electrode and a metal wiring portion,
2. The ferroelectric liquid crystal cell according to claim 1, wherein the metal wiring portion has a plurality of gaps that become wider as the distance from the driving source increases.
え、該金属配線部はほぼｎ等分の領域に分割されてお
り、前記電極に接続する駆動源から遠い側からＳ番目
（Ｓ＝1,2…ｎ）の領域の金属配線部には金属配線のな
い間隙部分が１つまたは複数個設けられており、Ｓ番目
の領域に設けられた該間隙部分のギャップgSが である、請求項１記載の強誘電性液晶セル。7. The electrode includes a transparent electrode and a metal wiring portion, the metal wiring portion being divided into substantially equal n regions, and an S-th (S) portion from a side farther from a driving source connected to the electrode. = 1, 2... N), one or more gap portions without metal wires are provided in the metal wiring portion, and the gap g S of the gap portion provided in the S-th region is provided. The ferroelectric liquid crystal cell according to claim 1, wherein
よびセグメント側電極であり、該コモン側電極もしくは
セグメント側電極のいずれかあるいはその両方は、前記
強誘電性液晶セルの表示部においてその長さ方向に抵抗
値によりほぼｈ等分の領域に分割され、前記RS＝h2／S2
・ROの関係を満たす請求項１記載の強誘電性液晶セル。8. The ferroelectric liquid crystal cell according to claim 8, wherein said electrodes are a common-side electrode and a segment-side electrode which are opposed to each other. In the vertical direction, the area is divided into substantially equal areas by the resistance value, and the above-mentioned R S = h 2 / S 2
2. The ferroelectric liquid crystal cell according to claim 1, which satisfies a relationship of R O.
配置し、その間に強誘電性液晶を挟持し、該電極を介し
て該強電性液晶の配向を制御する強誘電性液晶セルにお
いて、前記電極は透明電極と金属配線部を備え、該金属
配線部が該電極に接続する駆動源から遠ざかるにつれて
広くなる複数のギャップを有することにより、該電極は
該電極の長さ方向に該駆動源から遠ざかるにつれて単位
長さ当りの抵抗値が高くなるような抵抗分布を形成され
ていることを特徴とする強誘電性液晶セル。9. A ferroelectric liquid crystal cell in which a substrate on which stripe-shaped electrodes are formed is opposed to each other, a ferroelectric liquid crystal is interposed therebetween, and the orientation of the ferroelectric liquid crystal is controlled via the electrodes. The electrode includes a transparent electrode and a metal wiring portion, and the metal wiring portion has a plurality of gaps that become wider as the distance from the driving source connected to the electrode increases, so that the electrode is separated from the driving source in the length direction of the electrode. A ferroelectric liquid crystal cell characterized by forming a resistance distribution such that a resistance value per unit length increases as the distance increases.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63218526A JP2731916B2 (en) | 1988-09-02 | 1988-09-02 | Ferroelectric liquid crystal cell |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63218526A JP2731916B2 (en) | 1988-09-02 | 1988-09-02 | Ferroelectric liquid crystal cell |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0267521A JPH0267521A (en) | 1990-03-07 |
| JP2731916B2 true JP2731916B2 (en) | 1998-03-25 |
Family
ID=16721310
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63218526A Expired - Fee Related JP2731916B2 (en) | 1988-09-02 | 1988-09-02 | Ferroelectric liquid crystal cell |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2731916B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB2313224A (en) * | 1996-05-17 | 1997-11-19 | Sharp Kk | Ferroelectric liquid crystal device |
| GB2313226A (en) * | 1996-05-17 | 1997-11-19 | Sharp Kk | Addressable matrix arrays |
| JP4712937B2 (en) * | 2000-03-27 | 2011-06-29 | エーユー オプトロニクス コーポレイション | Liquid crystal display device, wiring structure, voltage supply method, and computer |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS55133084A (en) * | 1979-04-05 | 1980-10-16 | Tokyo Shibaura Electric Co | Plane display |
| JP2617709B2 (en) * | 1986-10-09 | 1997-06-04 | キヤノン株式会社 | Optical modulation element and driving method thereof |
| JPS63109421A (en) * | 1986-10-27 | 1988-05-14 | Fujitsu Ltd | Liquid crystal display |
-
1988
- 1988-09-02 JP JP63218526A patent/JP2731916B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0267521A (en) | 1990-03-07 |
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