JPH0750273B2 - Liquid crystal electro-optical device - Google Patents
Liquid crystal electro-optical deviceInfo
- Publication number
- JPH0750273B2 JPH0750273B2 JP60147400A JP14740085A JPH0750273B2 JP H0750273 B2 JPH0750273 B2 JP H0750273B2 JP 60147400 A JP60147400 A JP 60147400A JP 14740085 A JP14740085 A JP 14740085A JP H0750273 B2 JPH0750273 B2 JP H0750273B2
- Authority
- JP
- Japan
- Prior art keywords
- liquid crystal
- optical device
- thickness
- conductive film
- crystal electro
- 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 - Lifetime
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Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は液晶電気光学装置に関し、特にその製造方法に
関する。The present invention relates to a liquid crystal electro-optical device, and more particularly to a manufacturing method thereof.
本発明は液晶電気光学装置において、2枚の基板を重ね
合わせた時画素となる部分の液晶層厚が所望の厚さとな
る様に、ギヤツプ剤と電極を兼ねた適当な厚さの導電性
膜を少なくとも一方の基板上の画素部以外に設けたの
で、導電性膜の厚さを所望の液晶層厚とほぼ等しい厚さ
まで厚くすることができる。従つて、所望の液晶層厚が
薄い場合でも配線抵抗低減効果を最大限利用することが
でき、さらにギヤツプ剤散布の工程を省略することがで
きる。In the liquid crystal electro-optical device, the present invention is a conductive film having an appropriate thickness that also serves as a gearing agent and an electrode, so that when two substrates are superposed, the thickness of the liquid crystal layer in a pixel portion becomes a desired thickness. Is provided on at least one of the substrates other than the pixel portion, the thickness of the conductive film can be increased to a thickness substantially equal to a desired liquid crystal layer thickness. Therefore, even if the desired liquid crystal layer thickness is thin, the wiring resistance reducing effect can be utilized to the maximum extent, and the step of spraying the gearing agent can be omitted.
従来の液晶電気光学装置の構造は、ギヤツプ剤としてグ
ラスフアイバー、ビーズ、高分子フイルムなどを2枚の
基板間に挾んだものであつた。The structure of a conventional liquid crystal electro-optical device is such that a glass fiber, beads, a polymer film or the like as a gearing agent is sandwiched between two substrates.
しかし前述の従来技術では液晶層の厚さはギヤツプ剤の
直径と配線抵抗低減のために設けた導電性膜の厚さの和
となる。例として所望の液晶層の厚さが5μmの場合、
たとえばギヤツプ剤の直径を2μm、導電性膜の厚さを
3μmとすればよく電導性膜の厚さを十分厚くして配線
抵抗を低くすることができる。However, in the above-mentioned conventional technique, the thickness of the liquid crystal layer is the sum of the diameter of the gearing agent and the thickness of the conductive film provided for reducing the wiring resistance. As an example, if the desired liquid crystal layer thickness is 5 μm,
For example, the diameter of the gearing agent may be 2 μm and the thickness of the conductive film may be 3 μm. The thickness of the conductive film may be sufficiently thick to reduce the wiring resistance.
ところで、強誘電性スメクチツク液晶は液晶層厚を非常
に薄くすることによつて記憶効果、急峻なしきい特性、
高速応答というすぐれた特性を現わし、液晶電気光学装
置用の材料として高い可能性を持つている。これらの特
性が発現する液晶層厚は液晶材料に依存するが、良好な
特性を得るためには約1.5μm以下が望ましく、液晶層
厚が厚くなるにしたがつて、記憶効果およびしきい特性
の急峻性が低下する。また、強誘電性スメクチツク液晶
を用いた液晶電気光学装置のコントラスト比は式(1)
で表わされるクロスニコル間の透過光量Iから求めるこ
とができ、白色光を光源として用いる場合、△n=0.2
ならば液晶層厚dは1.4μm前後が最適となる。(現在
一般に使用されている強誘電性スメクチツク液晶の△n
の値は0.2前後である。) I=I0sin24θ・sin2(πdΔn/λ) (1) θ:液晶の分子軸と偏光子のなす角 △n:複屈折 d:液晶層厚 λ:入射光の波長 I0:入射光量 また、液晶電気光学装置のON,OFF状態をスイツチする周
期を短くするにしたがつて駆動電圧波形の周波数が高く
なり、配線抵抗と静電容量が高ければ駆動電圧波形が歪
んで駆動することができなくなる。そこで、所望の液晶
層の厚さが1μmの場合、従来の方法によつてギヤツプ
剤を使用すれば導電性膜の厚さは数1000Åとなり配線抵
抗を低減させる効果が小さくなる、という問題がある。By the way, the ferroelectric smectic liquid crystal has a memory effect, a sharp threshold characteristic, and
It exhibits excellent characteristics of high-speed response and has high potential as a material for liquid crystal electro-optical devices. The liquid crystal layer thickness at which these characteristics are expressed depends on the liquid crystal material, but it is desirable to be about 1.5 μm or less in order to obtain good characteristics. As the liquid crystal layer thickness increases, the memory effect and the threshold characteristic The steepness decreases. Further, the contrast ratio of the liquid crystal electro-optical device using the ferroelectric smectic liquid crystal is expressed by the formula (1).
It can be obtained from the transmitted light amount I between crossed Nicols, and when white light is used as the light source, Δn = 0.2
Then, the optimum liquid crystal layer thickness d is around 1.4 μm. ([Delta] n of the ferroelectric smectic liquid crystals that are currently used
The value of is around 0.2. ) I = I 0 sin 2 4θ ・ sin 2 (πdΔn / λ) (1) θ: angle between the molecular axis of liquid crystal and the polarizer Δn: birefringence d: liquid crystal layer thickness λ: wavelength of incident light I 0 : Incident light quantity In addition, the frequency of the drive voltage waveform becomes higher as the cycle of switching the ON / OFF state of the liquid crystal electro-optical device becomes shorter, and if the wiring resistance and capacitance are high, the drive voltage waveform is distorted and driven. Can't do it. Therefore, when the desired thickness of the liquid crystal layer is 1 μm, the use of a gearing agent according to the conventional method causes the thickness of the conductive film to be several thousand Å, which reduces the effect of reducing the wiring resistance. .
そこで本発明はこのような問題点を解決するもので、そ
の目的とするところは、所望の液晶層厚が非常に薄い場
合でも導電性膜による配線抵抗低減効果を最大限利用す
ることができ、ギヤツプ剤を散布する必要のない液晶電
気光学装置を提供するところにある。Therefore, the present invention solves such a problem, and an object thereof is to make maximum use of the wiring resistance reduction effect of the conductive film even when the desired liquid crystal layer thickness is very thin, An object of the present invention is to provide a liquid crystal electro-optical device that does not need to disperse a gearing agent.
本発明の液晶電気光学装置は、対向する内面に電極を有
する一対の基板間に液晶を挟持してなる液晶電気光学装
置において、少なくとも前記一方の電極上の画素となら
ない部分に、該電極と電気的接続され且つ前記基板間の
ギャップを制御するスペーサーを兼ねた導電性膜を形成
したことを特徴とする。The liquid crystal electro-optical device of the present invention is a liquid crystal electro-optical device in which a liquid crystal is sandwiched between a pair of substrates having electrodes on the inner surfaces facing each other, and at least a portion of the one electrode which is not a pixel is electrically connected to the electrode It is characterized in that a conductive film, which is also electrically connected and also serves as a spacer for controlling the gap between the substrates, is formed.
第1図に第1の実施例を示す。第1図(a)は本発明を
1/2デユーテイ液晶プリンターヘツドに応用した場合の
液晶光シヤツター部の平面図であり、第1図(b)は第
1図(a)のAA′における断面図である。下側基板17上
には走査電極11および絶縁層(SiO2)14を設け、その上
にPI,ナイロン,PVA等の配向処理膜18を設け、一方向に
ラビング処理を施してある。上側基板16上には信号電極
12を設け、さらに画素13以外の部分に導電性膜15を設け
てある。20は偏光板である。第1図(a)において二重
の斜線を施した液晶導入部21の導電性膜の厚さは所望の
液晶層厚より薄くなつており、その部分を通つて液晶19
が画素13の部分へ入つていく。FIG. 1 shows the first embodiment. FIG. 1 (a) illustrates the present invention.
FIG. 1 is a plan view of a liquid crystal light shutter section when applied to a 1/2 duty liquid crystal printer head, and FIG. 1 (b) is a sectional view taken along line AA ′ of FIG. 1 (a). A scan electrode 11 and an insulating layer (SiO 2 ) 14 are provided on a lower substrate 17, and an alignment treatment film 18 of PI, nylon, PVA or the like is provided on the scan electrode 11 and a rubbing treatment in one direction. Signal electrodes on the upper substrate 16
12 is provided, and a conductive film 15 is provided in a portion other than the pixel 13. 20 is a polarizing plate. In FIG. 1 (a), the thickness of the conductive film of the liquid crystal introduction portion 21 which is double shaded is thinner than the desired liquid crystal layer thickness, and the liquid crystal 19 passes through that portion.
Enters the portion of pixel 13.
透明電極、導電性膜としてそれぞれITOとニツケル(厚
さ0.95μm)を使用して第1図に示した構成の液晶プリ
ンターヘツドを作成した。la=180μm,lb=220μm,lc=
80μmである液晶材料としてMBRA−8を真空封入法によ
つて封入し、液晶の複屈折より求めた液晶層厚は1.01±
0.04μmであり、均一な液晶層厚の液晶プリンターヘツ
ドが得られた。A liquid crystal printer head having the structure shown in FIG. 1 was prepared by using ITO and nickel (thickness: 0.95 μm) as a transparent electrode and a conductive film, respectively. la = 180μm, lb = 220μm, lc =
MBRA-8, which is a liquid crystal material with a thickness of 80 μm, is sealed by the vacuum sealing method, and the liquid crystal layer thickness calculated from the birefringence of the liquid crystal is 1.01 ±
A liquid crystal printer head having a uniform liquid crystal layer thickness of 0.04 μm was obtained.
参考のために、第2図に従来技術による液晶プリンター
ヘツドの断面図を示す。ギヤツプ剤(ビーズ)22の直径
は小さいもので0.8μm程度のため、所望の液晶層厚が
1μmならば高導電性膜の厚さは0.2μm程度となる。
その厚さは第1の実施例における厚さの約1/5であり、
配線抵抗低減効果が薄れてしまう。For reference, FIG. 2 shows a cross-sectional view of a conventional liquid crystal printer head. Since the diameter of the gearing agent (bead) 22 is small, about 0.8 μm, the thickness of the highly conductive film is about 0.2 μm if the desired liquid crystal layer thickness is 1 μm.
Its thickness is about 1/5 of the thickness in the first embodiment,
The wiring resistance reduction effect is diminished.
第3図に第2の実施例を示す。本実施例では下側基板17
上の走査電極11の上にも導電性膜15としてニツケル膜を
設けさらに絶縁のためにSiO214を設けてある。走査電極
上および信号電極上のニツケル膜の厚さl3,l4をいずれ
も1.5μmとし、SiO2,ナイロンの厚さをそれぞれ1000
Å,800Å,la=180μm,lb=220μm,lc=40μmとして、M
BRA−8を使用して液晶プリンターヘツドを作成した。
本実施例での液晶層厚は3.10±0.03μmとなつた。A second embodiment is shown in FIG. In this embodiment, the lower substrate 17
A nickel film is provided as a conductive film 15 on the upper scanning electrode 11 and SiO 2 14 is provided for insulation. The thicknesses l 3 and l 4 of the nickel films on the scanning electrode and the signal electrode are both 1.5 μm, and the thicknesses of SiO 2 and nylon are 1000 respectively.
Å, 800Å, la = 180μm, lb = 220μm, lc = 40μm, M
A liquid crystal printer head was prepared using BRA-8.
The liquid crystal layer thickness in this example was 3.10 ± 0.03 μm.
第4図に第3の実施例を示す。ここではマトリクス型液
晶デイスプレイへの応用例を示す。導電性膜15はストラ
イプ状信号電極12の端に設けてあり、第4図(a)の2
重に斜線を施した円形の部分は第4図(b)に示すよう
に貝柱状になつている。導電性膜として銅を使用し、la
=430μm,lb=70μm,lc=30μm,l5=0.5μm,l6=70μm,
lc=30μm,l5=0.9μm,l6=0.6μmとし、MBRA−8を使
用して100×100マトリクス型液晶デイスプレイを作成し
た。液晶層厚は1.06±0.03μmとなつた。FIG. 4 shows a third embodiment. Here, an application example to a matrix type liquid crystal display is shown. The conductive film 15 is provided at the end of the stripe-shaped signal electrode 12, and is shown in FIG.
The circular portion with heavy diagonal lines has a scalloped shape as shown in FIG. 4 (b). Using copper as the conductive film, la
= 430 μm, lb = 70 μm, lc = 30 μm, l 5 = 0.5 μm, l 6 = 70 μm,
A 100 × 100 matrix liquid crystal display was prepared using MBRA-8 with lc = 30 μm, l 5 = 0.9 μm, l 6 = 0.6 μm. The liquid crystal layer thickness was 1.06 ± 0.03 μm.
本発明は液晶プリンターヘツド、マトリクス型液晶デイ
スプレイ以外の液晶電気光学装置へも応用することがで
き、液晶材料は強誘電性スメクチツク液晶に限定され
ず、液晶層厚も限定されない。The present invention can be applied to liquid crystal electro-optical devices other than the liquid crystal printer head and the matrix type liquid crystal display, and the liquid crystal material is not limited to the ferroelectric smectic liquid crystal and the liquid crystal layer thickness is not limited.
以上のような構成にすることによって、以下のような効
果が得られる。With the above configuration, the following effects can be obtained.
少なくとも一方の電極上にそって導電性膜を形成した
ので、電極の配線抵抗が低減する。又、導電性膜により
基板間のギャップも制御することができる。Since the conductive film is formed along at least one of the electrodes, the wiring resistance of the electrode is reduced. In addition, the gap between the substrates can be controlled by the conductive film.
配線抵抗が低減できるため、電圧パルスの遅延が小さ
くなる。従って、高画質の表示が得られる。Since the wiring resistance can be reduced, the delay of the voltage pulse is reduced. Therefore, high quality display can be obtained.
第1図(a)は第1の実施例における液晶プリンターヘ
ツドの平面図、第1図(b)は第1図(a)のAA′にお
ける断面図、第2図は従来技術を示す断面図、第3図は
第2の実施例における液晶プリンターヘツドの断面図、
第4図(a)は第3の実施例における液晶デイスプレイ
の平面図、第4図(b)は第4図(a)のAA′における
断面図である。 11……走査電極 12……信号電極 13……画素 14……絶縁層 15……導電性膜 16……上側基板 17……下側基板 18……配向処理膜 19……液晶 20……偏光板 21……液晶導入部 22……ギヤツプ剤FIG. 1 (a) is a plan view of the liquid crystal printer head in the first embodiment, FIG. 1 (b) is a sectional view taken along line AA 'of FIG. 1 (a), and FIG. 2 is a sectional view showing a conventional technique. FIG. 3 is a sectional view of the liquid crystal printer head in the second embodiment,
FIG. 4 (a) is a plan view of the liquid crystal display in the third embodiment, and FIG. 4 (b) is a sectional view taken along the line AA 'in FIG. 4 (a). 11 …… Scan electrode 12 …… Signal electrode 13 …… Pixel 14 …… Insulating layer 15 …… Conductive film 16 …… Upper substrate 17 …… Lower substrate 18 …… Alignment film 19 …… Liquid crystal 20 …… Polarization Plate 21 …… Liquid crystal introduction part 22 …… Gearing agent
Claims (1)
に液晶を挟持してなる液晶電気光学装置において、少な
くとも前記一方の電極上の画素とならない部分に、該電
極と電気的接続され且つ前記基板間のギャップを制御す
るスペーサーを兼ねた導電性膜を形成したことを特徴と
する液晶電気光学装置。1. A liquid crystal electro-optical device comprising a pair of substrates having electrodes on opposite inner surfaces and a liquid crystal sandwiched between the substrates, the liquid crystal electro-optical device being electrically connected to at least a portion of the one electrode which is not a pixel, A liquid crystal electro-optical device characterized in that a conductive film which also functions as a spacer for controlling a gap between the substrates is formed.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60147400A JPH0750273B2 (en) | 1985-07-04 | 1985-07-04 | Liquid crystal electro-optical device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60147400A JPH0750273B2 (en) | 1985-07-04 | 1985-07-04 | Liquid crystal electro-optical device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS628127A JPS628127A (en) | 1987-01-16 |
| JPH0750273B2 true JPH0750273B2 (en) | 1995-05-31 |
Family
ID=15429428
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60147400A Expired - Lifetime JPH0750273B2 (en) | 1985-07-04 | 1985-07-04 | Liquid crystal electro-optical device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0750273B2 (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2523486B2 (en) * | 1986-03-31 | 1996-08-07 | 松下電器産業株式会社 | Liquid crystal display panel and manufacturing method thereof |
| JP2526273B2 (en) * | 1988-07-04 | 1996-08-21 | スタンレー電気株式会社 | Liquid crystal display device |
| US5694188A (en) * | 1994-09-17 | 1997-12-02 | Kabushiki Kaisha Toshiba | Reflection type liquid crystal display device having comb-shaped wall electrode |
| US6465268B2 (en) | 1997-05-22 | 2002-10-15 | Semiconductor Energy Laboratory Co., Ltd. | Method of manufacturing an electro-optical device |
| JP2012198544A (en) * | 2012-04-16 | 2012-10-18 | Semiconductor Energy Lab Co Ltd | Display device |
| JP6927052B2 (en) * | 2018-01-10 | 2021-08-25 | 日本製鉄株式会社 | Metal strip straightening method and metal strip straightening device |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56122012A (en) * | 1980-03-03 | 1981-09-25 | Keiji Iimura | Tn-type liquid crystal cell |
| JPS5888722A (en) * | 1981-11-24 | 1983-05-26 | Keiji Iimura | Laminated electrooptic cell |
-
1985
- 1985-07-04 JP JP60147400A patent/JPH0750273B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS628127A (en) | 1987-01-16 |
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