JPH0210923B2 - - Google Patents

Info

Publication number
JPH0210923B2
JPH0210923B2 JP56080243A JP8024381A JPH0210923B2 JP H0210923 B2 JPH0210923 B2 JP H0210923B2 JP 56080243 A JP56080243 A JP 56080243A JP 8024381 A JP8024381 A JP 8024381A JP H0210923 B2 JPH0210923 B2 JP H0210923B2
Authority
JP
Japan
Prior art keywords
liquid crystal
film
voltage
mim
oxide film
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
Application number
JP56080243A
Other languages
Japanese (ja)
Other versions
JPS57195218A (en
Inventor
Shinji Morozumi
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 JP56080243A priority Critical patent/JPS57195218A/en
Publication of JPS57195218A publication Critical patent/JPS57195218A/en
Publication of JPH0210923B2 publication Critical patent/JPH0210923B2/ja
Granted 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
    • G02F1/136Liquid crystal cells structurally associated with a semi-conducting layer or substrate, e.g. cells forming part of an integrated circuit
    • G02F1/1362Active matrix addressed cells
    • G02F1/1365Active matrix addressed cells in which the switching element is a two-electrode device

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Liquid Crystal (AREA)
  • Engineering & Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Mathematical Physics (AREA)
  • Chemical & Material Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Devices For Indicating Variable Information By Combining Individual Elements (AREA)

Description

【発明の詳細な説明】 本発明は高デユーテイ駆動の液晶表示体を実現
するための金属―絶縁膜―金属(MIM)構造の
非線形素子に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a nonlinear element having a metal-insulating film-metal (MIM) structure for realizing a high-duty drive liquid crystal display.

従来液晶のダイナミツク駆動においては、その
デユーテイは1/16程度が限界であつたが、最近そ
の駆動デユーテイを改善する手段としてMIM素
子の如くの非線形素子を介して液晶を駆動する方
法が提案されている。例えば第1図に示すような
V―I特性を持つた受動素子を介して液晶を駆動
すると、液晶を点灯させる電圧VONが印加される
と素子側の実効抵抗が低く、液晶側の抵抗が高い
ので、印加された電圧の殆んどは液晶側にかか
る。又液晶を点灯させない電圧VOFFを印加すると
素子側の実効抵抗は液晶より高くなり、電圧は殆
んど液晶にかからなくなり、外部から印加する電
圧の比VON/VOFFに対し、液晶に実質的に印加さ
れる電圧の比ははるかに大きくなり、点灯と非点
灯の差、即ちマージンがかなり大きくなり、実効
的には駆動デユーテイが改善でき1/200程まで可
能となる。この非線形素子を実現するMIM素子
は第2図に示すような構造である。ガラス基板2
0上にTa膜、又はTaNを形成しパターンングし
てTa又はTaNの第1の金属電極21及びリード
部を形成後、陽極酸化によりTa2O5層22を形成
し、その後上部電極の第2の金属電極23を形成
する。Ta2O5層22は約500〜1000Åであり、こ
の絶縁膜中のトラツプを電子トンネル現象により
伝導することを利用して第1図の特性を実現す
る。このため絶縁膜層は十分に薄い必要がある。
In conventional dynamic driving of liquid crystals, the duty was limited to about 1/16, but recently a method of driving liquid crystals through nonlinear elements such as MIM elements has been proposed as a means of improving the driving duty. There is. For example, when a liquid crystal is driven through a passive element with VI characteristics as shown in Figure 1, when the voltage V ON that turns on the liquid crystal is applied, the effective resistance on the element side is low, and the resistance on the liquid crystal side is low. Since the voltage is high, most of the applied voltage is applied to the liquid crystal side. In addition, when a voltage V OFF that does not turn on the liquid crystal is applied, the effective resistance on the element side becomes higher than the liquid crystal, and almost no voltage is applied to the liquid crystal . Substantially, the ratio of the applied voltages becomes much larger, and the difference between lighting and non-lighting, that is, the margin, becomes considerably large, and the driving duty can be effectively improved to about 1/200. The MIM element that realizes this nonlinear element has a structure as shown in FIG. Glass substrate 2
After forming a Ta film or TaN on 0 and patterning it to form a Ta or TaN first metal electrode 21 and a lead part, a Ta 2 O 5 layer 22 is formed by anodic oxidation, and then a Ta 2 O 5 layer 22 is formed on the upper electrode. 2 metal electrodes 23 are formed. The Ta 2 O 5 layer 22 has a thickness of about 500 to 1000 Å, and the characteristics shown in FIG. 1 are realized by utilizing traps in this insulating film to be conducted by an electron tunneling phenomenon. For this reason, the insulating film layer needs to be sufficiently thin.

第3図はMIM素子30による液晶31の駆動
等価回路であり、VDが駆動電圧,VCは液晶の
共通電極の電圧,VMは実際に液晶の端子に印加
される電圧である。MIM素子は非線形抵抗RM
と容量CMで、液晶は抵抗RLと容量CLで表現で
きる。液晶31には液晶駆動電極を介して印加さ
れる。
FIG. 3 shows an equivalent circuit for driving the liquid crystal 31 by the MIM element 30, where VD is the driving voltage, VC is the voltage of the common electrode of the liquid crystal, and VM is the voltage actually applied to the terminals of the liquid crystal. MIM element has nonlinear resistance RM
and capacitance CM, and the liquid crystal can be expressed by resistance RL and capacitance CL. A voltage is applied to the liquid crystal 31 via a liquid crystal drive electrode.

第4図は実際の駆動波形であり、AがON時B
がOFF時である。電圧VDが0電位にもどつても
電圧VMは容量CLと抵抗RLの時定数が大きいの
で、印加された電圧をある程度維持できること
が、デユーテイ比を大きくできる理由であるが、
もし容量CMがCLに比し大きいと、VDが0電位
に戻つた時、電圧降下分△VM ON,△VM OFF
大きくなつてしまい、所望の働きをしなくなる。
Figure 4 shows the actual drive waveform, and when A is ON, B
is when it is OFF. Even when voltage VD returns to zero potential, voltage VM has a large time constant of capacitance CL and resistance RL, so the applied voltage can be maintained to a certain extent, which is why the duty ratio can be increased.
If the capacitance CM is larger than CL, when VD returns to 0 potential, the voltage drops △V M ON and △V M OFF will become large, and the desired function will not be achieved.

従つて、 CL≫CM としたいのであるが、実際に、液晶の駆動面積に
対し、Taの陽極酸化膜はεs=25もあるので、
MIM部分の面積を1/10000以下にする必要があ
る。
Therefore, we would like to make CL≫CM, but in reality, the Ta anodic oxide film has εs=25 compared to the driving area of the liquid crystal, so
The area of the MIM part needs to be 1/10000 or less.

例えば液晶駆動電極の大きさを300μm□ とする
とMIMの面積は3μm□となり現状のフオト・エ
ツチング技術では3μm□ のサイズを10cm大のガラ
ス全面で形成することは非常にむずかしい技術と
なり、実際にやろうとするとかなり高価な物につ
いてしまう。
For example, if the size of the liquid crystal drive electrode is 300μm□, the area of MIM is 3μm□, and with the current photo-etching technology, it is extremely difficult to form a 3μm□ size on the entire surface of a 10cm-sized glass. If you try, you'll end up with something quite expensive.

本発明はこのような欠点を改善する手段を提供
することを目的とし、実際にはMIMの絶縁膜と
して、誘電率の低いSiO,SiO2を使用する。
The present invention aims to provide a means for improving such drawbacks, and actually uses SiO, SiO 2 , which has a low dielectric constant, as the insulating film of the MIM.

但しMIM素子の絶縁膜は前述のようにある程
度の伝導率を維持するために、薄い必要があり、
そのためには緻密でピンホール等に欠陥の少ない
膜が要求される。従つてTa等の金属上に普通に
SiOやSiO2を形成すると、膜質が悪く、前記の条
件が満されない。従つて本発明はTa等の金属膜
上に、まずSi膜を形成し、次にこのSi膜を酸化す
ることにより、膜質のよいSiの酸化膜を得るもの
である。
However, as mentioned above, the insulating film of the MIM element needs to be thin in order to maintain a certain degree of conductivity.
For this purpose, a dense film with few defects such as pinholes is required. Therefore, it is commonly used on metals such as Ta.
If SiO or SiO 2 is formed, the film quality will be poor and the above conditions will not be met. Therefore, in the present invention, a Si oxide film of good quality is obtained by first forming a Si film on a metal film such as Ta, and then oxidizing the Si film.

第5図に本発明の具体例を示す。ガラス基板5
0上にTa等の金属膜の島51を形成する。次に
スパツタ、プラズマCVD法の低温デポジシヨン
により約100〜300ÅのSi膜52を形成する。
FIG. 5 shows a specific example of the present invention. glass substrate 5
0, an island 51 of a metal film such as Ta is formed. Next, a Si film 52 with a thickness of about 100 to 300 Å is formed by sputtering and plasma CVD at low temperature deposition.

次にこのSi膜52を酸化する。一つは負空チヤ
ンバ中に0.1〜10Torr程度のO2ガスを導入し、プ
ラズマ状態にて酸化する。他の手段はクエン酸等
の容液中で100V程度の電圧を印加して行なう陽
極酸化でもよい。これはSi膜を酸化して得られる
シリコン酸化膜が重要であるので、手段は類似の
方法であれば本発明の目的は達成される。その後
上部の金属層54を形成してMIM素子が形成さ
れる。
Next, this Si film 52 is oxidized. One is to introduce O 2 gas of about 0.1 to 10 Torr into a negative chamber and oxidize it in a plasma state. Another method may be anodic oxidation performed in a liquid such as citric acid by applying a voltage of about 100V. Since the silicon oxide film obtained by oxidizing the Si film is important, the object of the present invention can be achieved if the means are similar. Thereafter, a top metal layer 54 is formed to form the MIM device.

このようにして製作されたSiO又はSiO2の比誘
電率は3,5付近でありTa酸化物に対して約1/1
4である。従つて300μm□ の液晶ドツトに対し、
12μm□ となり従来技術で十分に作り易い大きさ
となる。この結果第4図における△VM ONと△
VM OFFが小さくなり液晶を駆動する実効電圧が
低下しないので十分高いデユーテイのダイナミツ
ク駆動を可能とする。
The dielectric constant of SiO or SiO 2 produced in this way is around 3.5, which is about 1/1 that of Ta oxide.
It is 4. Therefore, for a 300μm□ liquid crystal dot,
The size is 12 μm□, which is a size that is sufficiently easy to manufacture using conventional technology. As a result, △V M ON and △ in Figure 4
Since V M OFF is small and the effective voltage for driving the liquid crystal does not drop, dynamic drive with a sufficiently high duty is possible.

以上の如く、本発明の非線形素子は、MIM構
造を構成する絶縁膜はSi酸化膜であるので、液晶
駆動電極の面積を小さくすることが可能となり、
より高密度の画像表示装置の提供が可能となる。
なぜならば、Si酸化膜の誘電率は、他の絶縁物、
例えば五酸化タンタル、酸化アルミニウム、窒化
ケイ素等に較べて小さいので、非線形素子の面積
が同じ場合、絶縁膜の誘電率が小さいと非線形素
子の容量が小さくなり、それに伴つて液晶駆動電
極の面積を小さくすることができるからである。
As described above, in the nonlinear element of the present invention, since the insulating film constituting the MIM structure is a Si oxide film, it is possible to reduce the area of the liquid crystal drive electrode.
It becomes possible to provide an image display device with higher density.
This is because the dielectric constant of Si oxide film is different from that of other insulators.
For example, it is smaller than tantalum pentoxide, aluminum oxide, silicon nitride, etc., so if the area of the nonlinear element is the same, the capacitance of the nonlinear element will be smaller if the dielectric constant of the insulating film is smaller, and the area of the liquid crystal drive electrode will be reduced accordingly. This is because it can be made smaller.

更に、ただ単にSi酸化物をスパツタ法などで直
接形成しても、ピンホールのない緻密な膜を得る
ことができず、歩留りの点で実用上実現すること
ができなかつたのに対し、Si薄膜層を形成した後
に酸化してSi酸化膜を形成することにより、ピン
ホールのない緻密なSi酸化膜が得られ、上述の効
果を有する高密度の画像表示装置が歩留り良く実
現できるようにしたものである。
Furthermore, even if Si oxide was simply formed directly by sputtering, it was not possible to obtain a dense film without pinholes, and this was not practical in terms of yield. By forming a thin film layer and then oxidizing it to form a Si oxide film, a dense Si oxide film without pinholes can be obtained, making it possible to realize high-density image display devices with the above-mentioned effects with high yield. It is something.

更に、本発明によるSi酸化膜は、膜質が緻密で
あるので、非線形素子として耐圧が向上し、静電
気などによる高電圧に対して、素子が破壊されて
しまう不良が低減されるという効果を有する。
Furthermore, since the Si oxide film according to the present invention has a dense film quality, it has the effect of improving the withstand voltage as a nonlinear element and reducing the risk of element destruction due to high voltage caused by static electricity or the like.

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

第1図はMIM素子のV―I特性、第2図は
MIM素子の従来の構造、第3図はMIM素子で液
晶を駆動する等価回路、第4図はその動作波形、
第5図は本発明のMIM素子の製造工程図をそれ
ぞれ示す。 20,50……ガラス基板、21,23,5
1,54……Ta膜、23……Ta酸化物、52…
…Si膜又はSi酸化膜。
Figure 1 shows the VI characteristics of the MIM device, Figure 2 shows
The conventional structure of an MIM element, Figure 3 is an equivalent circuit for driving a liquid crystal with an MIM element, Figure 4 is its operating waveform,
FIG. 5 shows manufacturing process diagrams of the MIM device of the present invention. 20, 50...Glass substrate, 21, 23, 5
1,54...Ta film, 23...Ta oxide, 52...
...Si film or Si oxide film.

Claims (1)

【特許請求の範囲】[Claims] 1 絶縁基板上に第1の金属電極となる金属薄膜
を形成する工程、Si薄膜を沈着する工程、該Si薄
膜をほぼ酸化しSi酸化膜を形成する工程、該Si酸
化膜上に第2の金属電極を形成する工程からな
り、第1の金属電極―Si酸化膜―第2の金属電極
によりMIM構造の非線形素子が形成されてなる
ことを特徴とする液晶表示装置の製造方法。
1 A step of forming a metal thin film to become a first metal electrode on an insulating substrate, a step of depositing a Si thin film, a step of substantially oxidizing the Si thin film to form a Si oxide film, and a step of forming a second metal thin film on the Si oxide film. 1. A method for manufacturing a liquid crystal display device, comprising a step of forming a metal electrode, and comprising a first metal electrode, a Si oxide film, and a second metal electrode to form a nonlinear element with an MIM structure.
JP56080243A 1981-05-27 1981-05-27 Non-linear element Granted JPS57195218A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56080243A JPS57195218A (en) 1981-05-27 1981-05-27 Non-linear element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56080243A JPS57195218A (en) 1981-05-27 1981-05-27 Non-linear element

Publications (2)

Publication Number Publication Date
JPS57195218A JPS57195218A (en) 1982-11-30
JPH0210923B2 true JPH0210923B2 (en) 1990-03-12

Family

ID=13712878

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56080243A Granted JPS57195218A (en) 1981-05-27 1981-05-27 Non-linear element

Country Status (1)

Country Link
JP (1) JPS57195218A (en)

Also Published As

Publication number Publication date
JPS57195218A (en) 1982-11-30

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