JP2598255B2 - Electrode structure - Google Patents

Electrode structure

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Publication number
JP2598255B2
JP2598255B2 JP61239254A JP23925486A JP2598255B2 JP 2598255 B2 JP2598255 B2 JP 2598255B2 JP 61239254 A JP61239254 A JP 61239254A JP 23925486 A JP23925486 A JP 23925486A JP 2598255 B2 JP2598255 B2 JP 2598255B2
Authority
JP
Japan
Prior art keywords
potential
conductive film
conductors
electrode structure
electrode
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP61239254A
Other languages
Japanese (ja)
Other versions
JPS6394296A (en
Inventor
修三 金子
通 高橋
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 JP61239254A priority Critical patent/JP2598255B2/en
Priority to US07/105,012 priority patent/US4906072A/en
Publication of JPS6394296A publication Critical patent/JPS6394296A/en
Application granted granted Critical
Publication of JP2598255B2 publication Critical patent/JP2598255B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Liquid Crystal (AREA)
  • Liquid Crystal Display Device Control (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、電極構造体に関し、特に、液晶やエレクト
ロルミネセンス等の光学変調素子、もしくは電界を利用
して各種変調を行う手段などに用いられる電極への電位
付与方法に用いられる電極構造体に関する。
Description: TECHNICAL FIELD The present invention relates to an electrode structure, and more particularly to an electrode structure used for an optical modulation element such as liquid crystal or electroluminescence, or a means for performing various types of modulation using an electric field. The present invention relates to an electrode structure used in a method for applying a potential to an electrode to be used.

[開示の概要] 本明細書及び図面は、光学変調素子などに用いられる
電極への電位付与方法において、電極面を形成する導電
膜上に、複数の導電体を抵抗体を介して配設し、各導電
体に与えられる電位の組み合わせに対応する電位を各導
電体間の導電膜に付与することにより、区切られた電極
面の各全面に対してほぼ一様な電位を得ると共に、電源
の数を大幅に減少させることのできる技術を開示するも
のである。
[Summary of Disclosure] In this specification and the drawings, in a method for applying a potential to an electrode used for an optical modulation element or the like, a plurality of conductors are provided via a resistor on a conductive film forming an electrode surface. By applying a potential corresponding to a combination of potentials applied to the conductors to the conductive films between the conductors, a substantially uniform potential is obtained over each of the divided electrode surfaces, and the power supply It discloses a technique that can greatly reduce the number.

[従来の技術] 従来、液晶やエレクトロルミネセンス等の光学変調素
子、もしくは電界を利用して各種変調を行う手段などに
おける電極面への典型的な電位付与方法としては、第9
図に示すように、各電極100にそれぞれ信号供給線101を
接続し、それらの信号供給線101にそれぞれ所望の電圧
を与えることにより前記電極100の電位を設定するのが
普通である。
[Prior Art] Conventionally, as a typical method for applying an electric potential to an electrode surface in an optical modulation element such as a liquid crystal or electroluminescence, or a means for performing various kinds of modulation using an electric field, a ninth method is known.
As shown in the drawing, a signal supply line 101 is connected to each electrode 100, and a desired voltage is applied to each of the signal supply lines 101 to set the potential of the electrode 100.

[発明が解決しようとする問題点] しかしながら、上記従来の方法では、各電極100が独
立した構造で、しかもそれらの一方側の端部に信号供給
線101が接続されているので、例えば電極100がガラス基
板上に蒸着されたストライプ状の薄膜である場合など、
ストライプ途中での断裂等により、信号供給源102から
離れた側で電位が不安定になったり、また前記電極100
にそれぞれ所望の電位を付与するためには、各電位に対
応する電源103をそれぞれ備えておかなければならない
などの問題点があった。
[Problems to be Solved by the Invention] However, in the above-mentioned conventional method, each electrode 100 has an independent structure, and the signal supply line 101 is connected to one end thereof. Is a striped thin film deposited on a glass substrate,
Due to a rupture in the middle of the stripe or the like, the potential becomes unstable on the side away from the signal supply source 102, or the electrode 100
In order to apply a desired potential to each of the power supplies, a power source 103 corresponding to each potential must be provided.

本発明は、このような問題点に鑑みなされたもので、
特に区切られた電極面の各全面に対してほぼ一様な電位
を得ると共に、電源の数を大幅に減少させる電位付与方
法を実施するための電極構造体を提供することを目的と
する。
The present invention has been made in view of such problems,
In particular, it is an object of the present invention to provide an electrode structure for implementing a potential applying method for obtaining a substantially uniform potential over the entire divided electrode surface and greatly reducing the number of power supplies.

[問題点を解決するための手段] 本発明は、ストライプ状の導電膜の長手方向の両端部
に一対の導電体を設け、該一対の導電体にそれぞれ独立
的に複数の基準電位から選択される電位を与え、該一対
の導電体に与えられる基準電位の組合せにより、所定の
電位を上記導電膜に付与する電位付与方法に用いられる
電極構造体において、 上記導電膜と上記一対の導電体との間に、該導電膜の
幅方向にほぼ一様な電位が付与されるように、該導電膜
の抵抗よりも十分に高い抵抗を持つ抵抗体を介在させた
ことを特徴とする電極構造体である。
[Means for Solving the Problems] In the present invention, a pair of conductors is provided at both ends in the longitudinal direction of a striped conductive film, and each of the pair of conductors is independently selected from a plurality of reference potentials. An electrode structure used in a potential applying method of applying a predetermined potential to the conductive film by a combination of reference potentials applied to the pair of conductors, wherein the conductive film and the pair of conductors An electrode structure characterized by interposing a resistor having a resistance sufficiently higher than the resistance of the conductive film so that a substantially uniform potential is applied in the width direction of the conductive film. It is.

[作 用] 所望の間隔で、複数の導電体を導電膜上に配設するこ
とにより、導電膜等は一ライン毎に区切られることにな
る。一方、複数の導電体は、それぞれ高抵抗の抵抗体を
介して配設されているので、それぞれに独立した電位を
与えることができ、かつ電位の組み合わせに対応する電
位が導電体間の導電膜等に付与されることになる。
[Operation] By arranging a plurality of conductors on the conductive film at desired intervals, the conductive film and the like are separated for each line. On the other hand, since the plurality of conductors are provided via high-resistance resistors, respectively, independent potentials can be given to the respective conductors, and the potential corresponding to the combination of potentials is a conductive film between the conductors. And so on.

[実施例] 第1図は、本発明の電極構造体の一例を示す縦断面図
であり、第2図はその電極の平面図である。
Example FIG. 1 is a longitudinal sectional view showing an example of the electrode structure of the present invention, and FIG. 2 is a plan view of the electrode.

両図における電極構成は、導電膜(比較的低抵抗抵抗
膜)で形成された電極面1上に、比較的高抵抗の抵抗体
(誘電体)2を介して、複数の導電体3及び4が配設さ
れている。
The electrode configuration in both figures is such that a plurality of conductors 3 and 4 are formed on an electrode surface 1 formed of a conductive film (relatively low-resistance resistance film) via a relatively high-resistance resistor (dielectric) 2. Are arranged.

電極面1は、ガラス等の基体5上に、ITO,SnO2,In2O3
等の透明な薄膜もしくはAu等の金属薄膜により形成され
たものである。
The electrode surface 1 is made of ITO, SnO 2 , In 2 O 3
And the like, or a thin metal film such as Au.

抵抗体2は、比較的高抵抗の抵抗体であって、金属ド
ープしたSi,Se又はカーボンなどの導電性微粉を少量混
練したポリエステル等により形成されている。
The resistor 2 is a resistor having a relatively high resistance, and is formed of polyester or the like obtained by kneading a small amount of conductive fine powder such as metal-doped Si, Se or carbon.

導電体3及び4はAl,Au等で、抵抗体2上に形成され
る。
The conductors 3 and 4 are made of Al, Au or the like, and are formed on the resistor 2.

第3図及び第4図は、上記の電極構成において、電極
面1に所望の電位を付与する方法の説明図である。第3
図において、第1の導電体3は第1の電源6aに、第2の
導電体4は第2の電源6bに接続されていて、それぞれの
電圧をVa及びVbとする。ここで、説明を簡単にするた
め、2つの電源6a及び6bの電圧Va及びVbは共にV1,V2,V3
の3段階であるとする。
FIG. 3 and FIG. 4 are explanatory diagrams of a method of applying a desired potential to the electrode surface 1 in the above-described electrode configuration. Third
In the figure, a first conductor 3 is connected to a first power supply 6a, and a second conductor 4 is connected to a second power supply 6b, and their voltages are Va and Vb. Here, for simplicity of explanation, the voltage Va and Vb of the two power 6a and 6b are both V 1, V 2, V 3
It is assumed that there are three stages.

導電体3及び4の間の電位は、第4図に示すように、
抵抗体領域2a及び2bと電極面領域1aとで変化するが、印
加される電圧Va及びVbの組み合わせにより決定される。
即ち、VaとVbの組み合わせが共にV1のときV1、V1とV2
ときほぼ中間値のV12、V1とV3のとき中間値のV
13(V2)、共にV2のときV2、V2とV3のときはほぼ中間値
のV23、共にV3のときV3のいうように、電極面1の電位
が5通りに決定される。
The potential between the conductors 3 and 4 is, as shown in FIG.
Although it changes between the resistor regions 2a and 2b and the electrode surface region 1a, it is determined by the combination of the applied voltages Va and Vb.
Ie, V intermediate value when the V 12, V 1 and V 3 of the substantially intermediate value when V 1, V 1 and V 2 when the Va and Vb combination both V 1 of the
13 (V 2), V 23 approximately intermediate values when V 2, V 2 and V 3 when together V 2, as referred to both of V 3 when the V 3, the potential of the electrode surface 1 is five different It is determined.

以下、この電位が導電体3及び4の間で、電極面1の
全域にわたってほぼ一定に付与されるための条件を説明
する。
Hereinafter, conditions for applying this potential substantially uniformly between the conductors 3 and 4 over the entire area of the electrode surface 1 will be described.

第5図は、第3図に示した電極構成の等価回路であ
る。ここで、前記必要条件の1つは、抵抗体2の抵抗r2
が電極面1の抵抗r1よりも充分に大きいことで、そのよ
うに構成することにより、抵抗体2による大きな電圧降
下を起こし、電極面1での電圧降下を小さくして、ほぼ
一定の電位を得ることができる。
FIG. 5 is an equivalent circuit of the electrode configuration shown in FIG. Here, one of the necessary conditions is the resistance r 2 of the resistor 2.
By but sufficiently larger than the resistance r 1 of the electrode surface 1, by configuring as such, cause a large voltage drop due to the resistor 2, to reduce the voltage drop at the electrode surface 1, a substantially constant potential Can be obtained.

上記抵抗値の関係を更に具体的に説明すると、例え
ば、第6図に平面図で示すように、抵抗体2の間の電極
面1の幅がaで、そのシート抵抗値が100Ω/sq程度であ
る場合、電極面1と導電体3又は4とに挟まれる抵抗体
2の抵抗値は、長さaにわたって104Ω以上得られるこ
とが望ましい。また、この抵抗体2には電流によるジュ
ール熱が発生するが、これを最小限に防ぐためにも、抵
抗r2は適度に大きくした方がよい。このため、抵抗体2
としては耐圧の高い半導体もしくはそれよりも抵抗値の
高いものが使用に適している。
The relationship between the resistance values will be described more specifically. For example, as shown in a plan view in FIG. 6, the width of the electrode surface 1 between the resistors 2 is a, and the sheet resistance value is about 100 Ω / sq. In this case, it is desirable that the resistance value of the resistor 2 sandwiched between the electrode surface 1 and the conductor 3 or 4 be at least 10 4 Ω over the length a. Further, Joule heat due to current is generated in the resistor 2 , and in order to minimize this, it is preferable that the resistor r2 is appropriately increased. Therefore, the resistor 2
As such, a semiconductor having a high withstand voltage or a semiconductor having a higher resistance value than that is suitable for use.

次に必要な条件としては、前記導電体3又は4とし
て、電気抵抗の充分に低いものを使用することである。
このためには、金属のうち特に抵抗の低いもので、その
シート抵抗値が数+Ω/sq以下のものが望ましい。
The next necessary condition is that the conductor 3 or 4 should have a sufficiently low electric resistance.
For this purpose, it is desirable to use a metal having a particularly low resistance and a sheet resistance of several + Ω / sq or less.

上記の条件を満たすことにより、電極面1に対して安
定した一定の電位を付与することができ、特に、薄膜ス
トライプ状の電極面1の信号供給端から離れた位置に対
しても、前記導電体3又は4により安定した電位を与え
るので、電極面1の一部に断裂が発生しても電位が不安
定になることはない。
By satisfying the above conditions, a stable and constant potential can be applied to the electrode surface 1. In particular, even when the electrode surface 1 in the form of a thin-film stripe is away from the signal supply end, Since a more stable potential is applied to the body 3 or 4, even if a part of the electrode surface 1 is torn, the potential does not become unstable.

なお、第7図に示すように、信号供給端を導電体3及
び4に対して交互に逆方向に配置すると、上記の降下は
更に大きくなる。第7図は、本発明の電極構造体の応用
例を示す斜視図であって、例えば液晶やエレクトロルミ
ネセンス等の光学変調素子、その他の電界効果に基づく
各種変調素子の電極として良好な変調付与手段となる応
用例を示すもものである。第7図において、10は電界効
果により光学的もしくはその他の変調を呈する変調物質
であり、11は変調物質を介して本発明の電極構造体に対
向する対向電極である。変調物質10は、本発明により構
成された電極(1,2,3及び4)と対向電極11との間に形
成される電界により各種変調を行われるが、この変調を
有効に行うためには、抵抗体2の抵抗値を前記変調物質
10の電極間抵抗値よりも小さくすれば、変調物質10への
分圧を充分に得ることができる。また、前記変調物質10
の電極間容量との積即ち時定数が所望の変調応答周期よ
りも短くなるような抵抗を選択することにより、順調な
各種変調を行うことが望ましい。
Note that, as shown in FIG. 7, when the signal supply terminals are alternately arranged in opposite directions with respect to the conductors 3 and 4, the above-described drop is further increased. FIG. 7 is a perspective view showing an application example of the electrode structure of the present invention. For example, an optical modulation element such as a liquid crystal or an electroluminescence, and a good modulation application as an electrode of various modulation elements based on an electric field effect. This is an application example as a means. In FIG. 7, reference numeral 10 denotes a modulating substance which exhibits optical or other modulation by an electric field effect, and 11 denotes a counter electrode which faces the electrode structure of the present invention via the modulating substance. The modulation material 10 performs various types of modulation by an electric field formed between the electrodes (1, 2, 3, and 4) configured according to the present invention and the counter electrode 11, and in order to perform this modulation effectively, , The resistance of the resistor 2 to the modulation material
If the resistance value between the electrodes is smaller than 10, the partial pressure to the modulation substance 10 can be sufficiently obtained. Further, the modulation material 10
It is desirable to perform various types of smooth modulation by selecting a resistor whose product, that is, a time constant, is smaller than a desired modulation response cycle.

また、本発明の電極構造体は、第8図に示すように抵
抗体2の導電体3又は4がずれ合う形状で形成されても
差し支えない。
Further, the electrode structure of the present invention may be formed in a shape in which the conductors 3 or 4 of the resistor 2 are shifted as shown in FIG.

[発明の効果] 以上説明したように、本発明によれば、電極面を形成
する導電膜上に、複数の導電体を所望の間隔で抵抗体を
介して配設し、各導電体に与えられる電位の組み合わせ
に対応する電位を各導電体間の導電膜に付与することに
より、導電体で区切られた電極面の各全面に対してほぼ
一様な電位を得ると共に、電位を変調するにあたり電源
の数を大幅に減少させることができる。
[Effects of the Invention] As described above, according to the present invention, a plurality of conductors are provided at desired intervals via a resistor on a conductive film forming an electrode surface, and given to each conductor. By applying a potential corresponding to the combination of potentials applied to the conductive films between the conductors, a substantially uniform potential is obtained over each entire surface of the electrode surface divided by the conductors, and the potential is modulated. The number of power supplies can be greatly reduced.

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

第1図及び第2図は本発明の一実施例の縦断面図及び平
面図、第3図及び第4図は本発明にかかる電位付与の説
明図、第5図は実施例構成の等価回路図、第6図は電極
面の平面図、第7図は本発明の応用例の斜視図、第8図
は電極構成の別な実施例の縦断面図、第9図は従来例の
斜視図である。 1:導電膜又は低抵抗膜で形成された電極面、 2:抵抗体、 3,4:導電体、 5:基体、 6;,6.:電源。
1 and 2 are a longitudinal sectional view and a plan view of one embodiment of the present invention, FIGS. 3 and 4 are explanatory diagrams of potential application according to the present invention, and FIG. 5 is an equivalent circuit of the configuration of the embodiment. FIG. 6, FIG. 6 is a plan view of the electrode surface, FIG. 7 is a perspective view of an application example of the present invention, FIG. 8 is a longitudinal sectional view of another embodiment of the electrode configuration, and FIG. It is. 1: Electrode surface formed of conductive film or low resistance film, 2: Resistor, 3,4: Conductor, 5: Base, 6 ;, 6 .: Power supply.

Claims (4)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】ストライプ状の導電膜の長手方向の両端部
に一対の導電体を設け、該一対の導電体にそれぞれ独立
的に複数の基準電位から選択される電位を与え、該一対
の導電体に与えられる基準電位の組合せにより、所定の
電位を上記導電膜に付与する電位付与方法に用いられる
電極構造体において、 上記導電膜と上記一対の導電体との間に、該導電膜の幅
方向にほぼ一様な電位が付与されるように、該導電膜の
抵抗よりも十分に高い抵抗を持つ低抗体を介在させたこ
とを特徴とする電極構造体。
A pair of conductors are provided at both ends in the longitudinal direction of a stripe-shaped conductive film, and a potential selected from a plurality of reference potentials is applied to each of the pair of conductors independently. An electrode structure used in a potential applying method of applying a predetermined potential to the conductive film by a combination of reference potentials applied to a body, wherein the width of the conductive film is between the conductive film and the pair of conductors. An electrode structure comprising a low antibody having a resistance sufficiently higher than the resistance of the conductive film so that a substantially uniform potential is applied in the direction.
【請求項2】上記導電膜が透明導電膜である特許請求の
範囲第1項に記載の電極構造体。
2. The electrode structure according to claim 1, wherein said conductive film is a transparent conductive film.
【請求項3】上記抵抗体が、金属をドープしたSi,Se及
び導電性微粉を含むポリエステルから選択される材料か
らなる特許請求の範囲第1項に記載の電極構造体。
3. The electrode structure according to claim 1, wherein said resistor is made of a material selected from metal-doped Si, Se and polyester containing conductive fine powder.
【請求項4】上記導電体がA1又はAuである特許請求の範
囲第1項に記載の電極構造体。
4. The electrode structure according to claim 1, wherein said conductor is A1 or Au.
JP61239254A 1986-10-09 1986-10-09 Electrode structure Expired - Fee Related JP2598255B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP61239254A JP2598255B2 (en) 1986-10-09 1986-10-09 Electrode structure
US07/105,012 US4906072A (en) 1986-10-09 1987-10-06 Display apparatus and driving method for providing an uniform potential to the electrodes

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61239254A JP2598255B2 (en) 1986-10-09 1986-10-09 Electrode structure

Publications (2)

Publication Number Publication Date
JPS6394296A JPS6394296A (en) 1988-04-25
JP2598255B2 true JP2598255B2 (en) 1997-04-09

Family

ID=17042024

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61239254A Expired - Fee Related JP2598255B2 (en) 1986-10-09 1986-10-09 Electrode structure

Country Status (1)

Country Link
JP (1) JP2598255B2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61201217A (en) * 1985-03-04 1986-09-05 Nippon Telegr & Teleph Corp <Ntt> Liquid crystal cell

Also Published As

Publication number Publication date
JPS6394296A (en) 1988-04-25

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