JPH02165121A - Liquid crystal electrooptical element - Google Patents

Liquid crystal electrooptical element

Info

Publication number
JPH02165121A
JPH02165121A JP32023488A JP32023488A JPH02165121A JP H02165121 A JPH02165121 A JP H02165121A JP 32023488 A JP32023488 A JP 32023488A JP 32023488 A JP32023488 A JP 32023488A JP H02165121 A JPH02165121 A JP H02165121A
Authority
JP
Japan
Prior art keywords
transparent electrodes
liquid crystal
transparent
patterns
transparent 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.)
Pending
Application number
JP32023488A
Other languages
Japanese (ja)
Inventor
Minoru Yazaki
矢崎 稔
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson Corp
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 Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP32023488A priority Critical patent/JPH02165121A/en
Publication of JPH02165121A publication Critical patent/JPH02165121A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333Constructional arrangements; Manufacturing methods
    • G02F1/1335Structural association of cells with optical devices, e.g. polarisers or reflectors
    • G02F1/133509Filters, e.g. light shielding masks
    • G02F1/133512Light shielding layers, e.g. black matrix
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333Constructional arrangements; Manufacturing methods
    • G02F1/1343Electrodes
    • G02F1/134309Electrodes characterised by their geometrical arrangement
    • G02F1/134336Matrix
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333Constructional arrangements; Manufacturing methods
    • G02F1/1343Electrodes
    • G02F1/13439Electrodes characterised by their electrical, optical, physical properties; materials therefor; method of making

Abstract

PURPOSE:To prevent the light leakage between transparent electrodes and to lower resistance by providing auxiliary electrodes in contact with the transparent electrodes to approximately cover the spacings between the transparent electrodes. CONSTITUTION:The liquid crystal cell is constituted by applying electroless nickel plating in the form of patterns on substrates 12, 13 consisting of glass and forming electrically conductive layers 15 thereon. The electroless nickel patterns are so disposed as to cover the positions between the transparent electrodes 14 when viewed through the cell. Further, a metal surface is exposed while a resin layer 18 is formed and the transparent electrodes 14 are formed thereon. The metallic patterns 15 are formed at the same pitch as the pitch of the transparent electrode patterns 14 at this time. The resulted liquid crystal electrooptical element is free from the light leakage between the transparent electrodes and, therefore, exhibits an excellent contrast characteristic and further the sheet resistance of the transparent electrodes is extremely low.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、液晶電気光学素子に関し、特に低抵抗と透明
電極間の光漏れ防止を兼ねた電極構造に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a liquid crystal electro-optical device, and more particularly to an electrode structure that has low resistance and prevents light leakage between transparent electrodes.

[従来の技術] 近年、FSC(強誘電性スメクチック液晶)、DSTN
 (ダブルス−バーツイスト型液晶)等の出現により、
液晶電気光学素子の特性は飛躍的に向上した。これに伴
い表示容量の増加、大型化がもたらされ液晶電気光学素
子の電極パターンは、微細でかつ長いものとなった。従
って電極抵抗は従来以上に低抵抗であることが要求され
る。またこれ等大容量タイプの液晶電気光学素子は、そ
の動作原理上、電極間の隙間において光漏れを起こし易
い性質を有している。即ち、FSCにおいては双安定性
のために電界のかがらない電極間では、光を透過するド
メインと透過しないドメインが共存する、一方DSTN
においては電極段差が光漏れとなる。従来、液晶電気光
学素子の透明電極としては、酸化インジウム、酸化スズ
の混合物をスパッタまたは蒸着により薄膜形成した後、
所望形状にパターン化したもの、または第2図に示した
如く透明電極上に一部金属パターンを設け、低抵抗化を
計る構造が提示されている。
[Prior art] In recent years, FSC (ferroelectric smectic liquid crystal), DSTN
With the advent of (double bar twist type liquid crystal) etc.
The characteristics of liquid crystal electro-optical elements have improved dramatically. This has led to increased display capacity and larger sizes, and the electrode patterns of liquid crystal electro-optic elements have become finer and longer. Therefore, the electrode resistance is required to be lower than before. Moreover, these large-capacity type liquid crystal electro-optical elements have a property that light leakage occurs easily in the gaps between electrodes due to their operating principle. That is, in FSC, between the electrodes where no electric field is applied due to bistability, domains that transmit light and domains that do not transmit light coexist; on the other hand, in DSTN
In this case, the electrode level difference causes light leakage. Conventionally, transparent electrodes for liquid crystal electro-optical elements have been made by forming a thin film of a mixture of indium oxide and tin oxide by sputtering or vapor deposition, and then
Structures have been proposed in which a metal pattern is patterned into a desired shape, or a metal pattern is partially provided on a transparent electrode, as shown in FIG. 2, in order to reduce the resistance.

[発明が解決しようとする課題] しかし、上記従来方法では透明電極上に、金属パターン
を設ける六め、低抵抗化には効果のあるものの、電極間
の光漏れを防止できないという問題点があった。
[Problems to be Solved by the Invention] However, in the above conventional method, although providing a metal pattern on the transparent electrode is effective in reducing resistance, there is a problem in that light leakage between the electrodes cannot be prevented. Ta.

[課題を解決するための手段] 本発明の液晶電気光学素子は、透明電極を備えた2枚の
基板間に液晶を挟持してなる液晶電気光学素子に於て、
前記基板の少なくとも一方の基板の透17/J電極の下
層の一部に、それぞれの透明電極に沿って設けられた導
電体からなる補助電極を前記透明電極と接触して設け、
しかも前記透明電極と接する面と逆側の面は、透明電極
間の隙間を略覆うことのできる大きさであり、しかも前
記透明電極間の隙間を略覆うことのできる大きさの補助
電極部は光透過を防止することを特徴とする。
[Means for Solving the Problems] The liquid crystal electro-optical element of the present invention is a liquid crystal electro-optical element in which a liquid crystal is sandwiched between two substrates each having a transparent electrode.
An auxiliary electrode made of a conductor is provided along each transparent electrode on a part of the lower layer of the transparent 17/J electrode of at least one of the substrates, and is in contact with the transparent electrode,
Moreover, the surface opposite to the surface in contact with the transparent electrodes has a size that can substantially cover the gap between the transparent electrodes, and the auxiliary electrode portion has a size that can substantially cover the gap between the transparent electrodes. It is characterized by preventing light transmission.

以下、実施例により本発明の詳細を示す。Hereinafter, the details of the present invention will be shown by examples.

[実施例] 第1図に、本発明の実施例における液晶電気光学素子の
断面略図を示す。図中、10は液晶セル、11は偏光板
である。液晶セルはガラスからなる基板12.13上に
パターン状に無電界ニッケルメッキを施した後、フォト
レジストパターンにより約30μm幅で電界ニッケルメ
ッキを約15μm塗布し、導電体層15を形成した。尚
この時、無電界ニッケルパターンは透過して見たとき透
明電極14の間の位置を覆うように配置した。更に、そ
の上にスクリーン印刷法でポリイミド樹脂を約15μm
塗布、焼成した後、この基板をPVA常磐上でラッピン
グした後、更に発泡ウレタン常襲上でアルミナ研暦剤を
用いて研磨して樹脂418を形成しながら金属面を露出
させた。この面上にスパッタ法によりIT○を約200
0人設けた後フォトマスクにより約300μm幅でパタ
ーニングし、透明電i14を形成した。尚、この時金属
パターン15は透明電極パターン14と同一ピッチで形
成されている。更に、この上にポリイミドからなる配向
膜を殺はラビングして液晶セル10を組み立て、液晶1
6を封入した。得られた液晶電気光学素子は、透明電極
間の光漏れが無いため優れたコントラスト特性を示し、
更に透明電極のシート抵抗は、およそ1.1Ω/口に相
当し今回用いた透明電極のシート抵抗およそ20Ω/口
に比べ極めて低い抵抗となった。又、この値は従来透明
電極上金fX電極に比べても金属部分の体摂が大きくで
きるため、約1/10程度の抵抗となり、著しく低抵抗
化ができた。
[Example] FIG. 1 shows a schematic cross-sectional view of a liquid crystal electro-optical element in an example of the present invention. In the figure, 10 is a liquid crystal cell, and 11 is a polarizing plate. For the liquid crystal cell, electroless nickel plating was applied in a pattern on substrates 12 and 13 made of glass, and then electrolytic nickel plating was applied to a thickness of about 15 μm in a width of about 30 μm using a photoresist pattern to form a conductive layer 15. At this time, the electroless nickel pattern was placed so as to cover the positions between the transparent electrodes 14 when viewed through the transparent electrodes. Furthermore, about 15 μm of polyimide resin is applied on top of it by screen printing method.
After coating and firing, this substrate was lapped with PVA tokiwa, and then polished using alumina polishing agent on foamed urethane to form resin 418 while exposing the metal surface. Approximately 200 IT○ was applied onto this surface by sputtering.
After 0 persons were placed, patterning was performed with a width of about 300 μm using a photomask to form a transparent electrode i14. Note that, at this time, the metal patterns 15 are formed at the same pitch as the transparent electrode patterns 14. Furthermore, an alignment film made of polyimide is rubbed on top of this to assemble the liquid crystal cell 10, and the liquid crystal 1
6 was enclosed. The obtained liquid crystal electro-optical device exhibits excellent contrast characteristics because there is no light leakage between transparent electrodes.
Furthermore, the sheet resistance of the transparent electrode was approximately 1.1 Ω/hole, which was extremely low compared to the sheet resistance of the transparent electrode used this time, which was approximately 20 Ω/hole. Moreover, this value is about 1/10 of the resistance because the metal part can be larger than the conventional gold fX electrode on a transparent electrode, and the resistance can be significantly lowered.

上記実施例は、本発明の一部を示すもので、導電体とし
てニッケルで示したが他の金属、導電性樹脂または、そ
れ等を組み合わせても同様に可能である。更に金属、樹
脂の形成方法、厚み、研磨研削条件等は、任意に選択さ
れるもので、本実施例条件に限定されるものではなく、
又透明電極の下の樹脂層を着色してカラーフィルタとし
て用いた場合でも同様に可能である。
The above embodiments show a part of the present invention, and although nickel is used as the conductor, other metals, conductive resins, or a combination of these may be used as well. Furthermore, the method of forming metal and resin, the thickness, polishing and grinding conditions, etc. can be selected arbitrarily and are not limited to the conditions of this example.
It is also possible to use the resin layer under the transparent electrode as a color filter by coloring it.

[発明の効果] 以上述べたように本発明によれば、液晶電気光学素子の
透明電極間の光漏れを防止してしかも低抵抗化が可能で
あるため、表示特性の憬れた、大型で大容量の液晶電気
光学素子が容易に得られる効果を有する。
[Effects of the Invention] As described above, according to the present invention, it is possible to prevent light leakage between the transparent electrodes of a liquid crystal electro-optic element and also to reduce the resistance. A capacitive liquid crystal electro-optical element has an effect that can be easily obtained.

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

第1図は、本発明の実施例における液晶電気光学素子の
断面略図を示す。 第2図は従来の液晶電気光学素子の断面略図を示す。 106 液晶セル 11、偏光板 126 基板 13、基板 14、透明電極 15、導電体層 16、液晶 17、シール材 18、樹脂層 以上 第2図
FIG. 1 shows a schematic cross-sectional view of a liquid crystal electro-optic element in an embodiment of the present invention. FIG. 2 shows a schematic cross-sectional view of a conventional liquid crystal electro-optical element. 106 Liquid crystal cell 11, polarizing plate 126 Substrate 13, substrate 14, transparent electrode 15, conductor layer 16, liquid crystal 17, sealant 18, resin layer and above FIG.

Claims (1)

【特許請求の範囲】[Claims] (1)透明電極を備えた2枚の基板間に液晶を挟持して
なる液晶電気光学素子に於て、前記基板の少なくとも一
方の基板の透明電極の下層の一部に、それぞれの透明電
極に沿って設けられた導電体からなる補助電極を前記透
明電極と接触して設け、しかも前記透明電極と接する面
と逆側の面は、透明電極間の隙間を略覆うことのできる
大きさであり、しかも前記透明電極間の隙間を略覆うこ
とのできる大きさの補助電極部は光透過を防止すること
を特徴とする液晶電気光学素子。
(1) In a liquid crystal electro-optical device in which a liquid crystal is sandwiched between two substrates each having a transparent electrode, a portion of the lower layer of the transparent electrode of at least one of the substrates is provided with a portion of each transparent electrode. An auxiliary electrode made of a conductor provided along the transparent electrode is provided in contact with the transparent electrode, and the surface opposite to the surface in contact with the transparent electrode has a size that can substantially cover the gap between the transparent electrodes. In addition, the auxiliary electrode portion is sized to substantially cover the gap between the transparent electrodes, and prevents light transmission.
JP32023488A 1988-12-19 1988-12-19 Liquid crystal electrooptical element Pending JPH02165121A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32023488A JPH02165121A (en) 1988-12-19 1988-12-19 Liquid crystal electrooptical element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32023488A JPH02165121A (en) 1988-12-19 1988-12-19 Liquid crystal electrooptical element

Publications (1)

Publication Number Publication Date
JPH02165121A true JPH02165121A (en) 1990-06-26

Family

ID=18119222

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32023488A Pending JPH02165121A (en) 1988-12-19 1988-12-19 Liquid crystal electrooptical element

Country Status (1)

Country Link
JP (1) JPH02165121A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04350820A (en) * 1991-05-29 1992-12-04 Nec Corp Liquid crystal element
EP0814142A2 (en) * 1996-06-17 1997-12-29 Canon Kabushiki Kaisha Liquid crystal device and liquid crystal apparatus

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04350820A (en) * 1991-05-29 1992-12-04 Nec Corp Liquid crystal element
EP0814142A2 (en) * 1996-06-17 1997-12-29 Canon Kabushiki Kaisha Liquid crystal device and liquid crystal apparatus
EP0814142A3 (en) * 1996-06-17 1998-12-16 Canon Kabushiki Kaisha Liquid crystal device and liquid crystal apparatus
EP1088877A2 (en) * 1996-06-17 2001-04-04 Canon Kabushiki Kaisha Liquid crystal device and liquid crystal apparatus
EP1088877A3 (en) * 1996-06-17 2001-04-11 Canon Kabushiki Kaisha Liquid crystal device and liquid crystal apparatus
US6252641B1 (en) 1996-06-17 2001-06-26 Canon Kabushiki Kaisha Liquid crystal device and liquid crystal apparatus

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