JPH0282579A - Manufacturing method of thin film transistor - Google Patents
Manufacturing method of thin film transistorInfo
- Publication number
- JPH0282579A JPH0282579A JP63234021A JP23402188A JPH0282579A JP H0282579 A JPH0282579 A JP H0282579A JP 63234021 A JP63234021 A JP 63234021A JP 23402188 A JP23402188 A JP 23402188A JP H0282579 A JPH0282579 A JP H0282579A
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- gate insulating
- insulating film
- film transistor
- substrate
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/60—Insulated-gate field-effect transistors [IGFET]
- H10D30/67—Thin-film transistors [TFT]
- H10D30/6704—Thin-film transistors [TFT] having supplementary regions or layers in the thin films or in the insulated bulk substrates for controlling properties of the device
- H10D30/6713—Thin-film transistors [TFT] having supplementary regions or layers in the thin films or in the insulated bulk substrates for controlling properties of the device characterised by the properties of the source or drain regions, e.g. compositions or sectional shapes
Landscapes
- Thin Film Transistor (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明はアクティブマトリックス方式の液晶デイスプレ
ィや、イメージセンサや3次元集積回路などに応用され
る薄膜トランジスタに関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a thin film transistor applied to active matrix liquid crystal displays, image sensors, three-dimensional integrated circuits, and the like.
従来の薄膜トランジスタは、例えばJAPANDISP
LAY ’86の1986年p196〜p199に示
される様な構造であった。この構造を一般化して、その
概要を第2図に示す、 (a)図は上視図であり(b)
図はAA’における断面図である。ガラス、石英、サフ
ァイア等の絶縁基板201上に、ドナーあるいは、アク
セプタとなる不純物を添加した多結晶シリコン薄膜から
成るソース電極202及びドレイン電極203が形成さ
れている。これに接して、ソース電極204とドレイン
電極205が設けられており、更にソース電極202及
びドレイン電極203の上側で接し両者を結ぶように多
結晶シリコン薄膜から成る半導体層206が形成されて
いる。これらを被覆するようにゲート絶縁膜207が熱
CVD法により形成されている。更にこれに接しゲート
電極208が設けられている。Conventional thin film transistors are, for example, JAPANDISP
It had a structure as shown in LAY '86, 1986, pages 196-199. This structure is generalized and its outline is shown in Figure 2. (a) Figure is a top view, (b)
The figure is a cross-sectional view at AA'. A source electrode 202 and a drain electrode 203 are formed on an insulating substrate 201 made of glass, quartz, sapphire, etc., which are made of a polycrystalline silicon thin film doped with impurities to serve as donors or acceptors. A source electrode 204 and a drain electrode 205 are provided in contact with this, and a semiconductor layer 206 made of a polycrystalline silicon thin film is further formed in contact with the upper side of the source electrode 202 and the drain electrode 203 to connect them. A gate insulating film 207 is formed by thermal CVD to cover these. Furthermore, a gate electrode 208 is provided in contact with this.
しかし、従来の薄膜トランジスタは次のような問題点を
有していた。However, conventional thin film transistors have the following problems.
熱CVD法により基板の強度を、400°Cに保持し、
ゲート絶縁膜を形成するため、基板として#7059
(コーニング社製)を使用した場合、ゲート絶縁膜の熱
膨張係数が約6xICM’と小さいのに対し、#705
9基板は46xlO−マと大きい為、ゲート絶縁膜形成
後基板の反り、変形、ゲート絶縁膜のひび割れ等が生じ
、薄膜トランジスタの欠陥の原因となっていた。又基板
を大型化した場合、上記の現象が顕著に見られ基板の大
型化の大きな防げとなっていた。The strength of the substrate is maintained at 400°C by thermal CVD method,
#7059 as a substrate to form a gate insulating film
(manufactured by Corning), the thermal expansion coefficient of the gate insulating film is as small as approximately 6xICM', whereas #705
Since the No. 9 substrate was as large as 46xlO-ma, warpage and deformation of the substrate after formation of the gate insulating film, cracking of the gate insulating film, etc. occurred, which caused defects in the thin film transistor. Furthermore, when the size of the substrate is increased, the above-mentioned phenomenon becomes noticeable, and the increase in size of the substrate is largely prevented.
又熱CVD法によりゲート絶縁膜を形成すると形成され
た絶1IIIの膜質が悪く、薄膜トランジスタの表面電
荷密度が約I X 10”am−’と大きく、信頼性を
著しく低下させていた。Furthermore, when a gate insulating film is formed by thermal CVD, the quality of the formed insulating film is poor, and the surface charge density of the thin film transistor is as high as about I x 10"am-', which significantly reduces reliability.
熱CVD法は、基板をセットする治具や、チャンバーに
付着した5101の膜質が悪く、容易に剥離してパーテ
ィクルが発生し、形成したゲート絶縁膜にピンホールが
生じ、薄膜トランジスタの欠陥の原因となっていた。In the thermal CVD method, the quality of the 5101 film adhering to the jig for setting the substrate or the chamber is poor, and it easily peels off, generating particles and causing pinholes in the formed gate insulating film, which can cause defects in thin film transistors. It had become.
本発明は、このような問題点を解決するものであり、そ
の目的とするところは、信頼性の高い薄膜トランジスタ
を大面積にわたり、低欠陥で提供することにある。The present invention is intended to solve these problems, and its purpose is to provide a highly reliable thin film transistor over a large area with fewer defects.
本発明の薄膜トランジスタは、ソース電極及びドレイン
電極の断面形状のテーパー角が60度以下であり、ゲー
ト絶縁膜をECRプラズマCVD法で形成したことを特
徴とする。The thin film transistor of the present invention is characterized in that the taper angle of the cross-sectional shape of the source electrode and the drain electrode is 60 degrees or less, and the gate insulating film is formed by the ECR plasma CVD method.
以下実施例に基づいて本発明の詳細な説明する。 The present invention will be described in detail below based on Examples.
第1図に本発明による薄膜トランジスタの構造を示す。FIG. 1 shows the structure of a thin film transistor according to the present invention.
第1図(a)に示す様にガラス、石英、サファイア等の
絶縁基板101上にドナーあるいはアクセプタとなる不
純物を添加した多結晶シリコン、非晶質シリコン等のシ
リコン薄膜を減圧CVD法、プラズマCVD法等のCV
D法あるいは、真空蒸着法、スパッタ法により形成する
0次にフォトリソグラフィー技術により所定の形状にフ
ォトレジスト膜を形成し、 ドライエツチング技術によ
りシリコン薄膜をエツチングし、ソース電極102及び
ドレイン電極103を形成する。エツチングに使用した
ガスはCFaガスと02ガスの混合ガスであり、CFa
lOp比を小さくすればテーパー角104は小さく、逆
にCF al Oe比を大きくすればテーパー角104
は大きくなる。CF*10e比を厳密に制御すれば再現
性よくテーパー角104を調整することができる。CF
4102=0.25とし60度のテーパー角104が得
られた。ソース電極102及びドレイン電極103の膜
厚は500〜5000Aが望ましい。As shown in FIG. 1(a), a silicon thin film of polycrystalline silicon, amorphous silicon, etc. doped with impurities to serve as donors or acceptors is deposited on an insulating substrate 101 made of glass, quartz, sapphire, etc. by low pressure CVD or plasma CVD. CV of law etc.
A photoresist film is formed in a predetermined shape using zero-order photolithography technology using the D method, vacuum evaporation method, or sputtering method, and the silicon thin film is etched using dry etching technology to form a source electrode 102 and a drain electrode 103. do. The gas used for etching was a mixed gas of CFa gas and 02 gas.
If the lOp ratio is decreased, the taper angle 104 is decreased, and conversely, if the CF al Oe ratio is increased, the taper angle 104 is decreased.
becomes larger. By strictly controlling the CF*10e ratio, the taper angle 104 can be adjusted with good reproducibility. C.F.
4102=0.25, and a taper angle 104 of 60 degrees was obtained. The film thickness of the source electrode 102 and the drain electrode 103 is preferably 500 to 5000 Å.
第1図(b)に示す様に金属、透明導電膜等から成るソ
ース配線105及びドレイン配線106をスパッタ法あ
るいは真空蒸着法により形成し、多結晶シリコンあるい
は非晶質シリコン等のシリコン薄膜から成る半導体層1
07を減圧CVD法、プラズマCVD法等のCVD法あ
るいは真空蒸着法により形成する。その膜厚は200O
A以下が望ましい0次に、ECRプラズマCVD法によ
り5ide、SiNx等のゲート絶縁膜108を形成す
る。使用した装置の概略を第3図に示す、主要部は、プ
ラズマ室303と試料室310で構成されプラズマ室3
03に石英窓311を通して、周波数2.45GHz、
1107−600Wのマイクロ波307が、外周の磁気
コイル305により磁界が供給できる。プラズマ室内で
マイクロ波と磁界の相互作用で発生した高活性プラズマ
とイオン流304は発散磁界によって試料室310へ輸
送され、気相反応・表面反応を経て、絶縁基板301上
に膜が形成される。5insを形成する場合ガスライン
306より15 *ccnの酸素ガスが、ガスライン3
08より61tellの5iHnガスを供給した。この
時の圧力は6.0xlO−’Torrで、形成速度は約
670 A / m i nであった。その膜厚は10
00〜5000Aが望ましい、試料台302に固定され
た基板301は、高活性プラズマとイオン流の衝撃効果
により、低温で良質の膜が得られる一方ECRプラズマ
CVD法は高活性プラズマ流の強い方向性のゆえに、段
差側壁部の脆弱さが顕著となる。この結果ゲート絶縁膜
の破壊電圧を極端に低くしてしまう、破壊電界強度とテ
ーパー角の関係を第5図に示す、この破壊電界強度はテ
ーパー角に大きく依存しており、テーパー角を60度以
下にすると6 M V / c mという大きな値が得
られた。As shown in FIG. 1(b), source wiring 105 and drain wiring 106 made of metal, transparent conductive film, etc. are formed by sputtering or vacuum evaporation, and are made of silicon thin film such as polycrystalline silicon or amorphous silicon. semiconductor layer 1
07 is formed by a CVD method such as a low pressure CVD method or a plasma CVD method, or a vacuum evaporation method. The film thickness is 200O
Next, a gate insulating film 108 of 5ide, SiNx, etc. is formed by the ECR plasma CVD method, which is preferably less than A. The outline of the apparatus used is shown in Fig. 3.The main parts are a plasma chamber 303 and a sample chamber 310.
03 through the quartz window 311, the frequency is 2.45 GHz,
A microwave 307 of 1107-600 W can be supplied with a magnetic field by a magnetic coil 305 on the outer periphery. Highly active plasma and ion flow 304 generated by the interaction of microwaves and magnetic fields in the plasma chamber are transported to the sample chamber 310 by the divergent magnetic field, and a film is formed on the insulating substrate 301 through gas phase reaction and surface reaction. . When forming 5ins, 15*ccn of oxygen gas is supplied from the gas line 306 to the gas line 3.
From 08, 61 tell of 5iHn gas was supplied. The pressure at this time was 6.0xlO-'Torr, and the formation rate was about 670 A/min. Its film thickness is 10
The substrate 301 fixed on the sample stage 302, which is preferably 00 to 5000 A, can obtain a high-quality film at low temperature due to the impact effect of the highly active plasma and ion flow, while the ECR plasma CVD method has a strong directionality of the highly active plasma flow. Therefore, the fragility of the step side wall becomes remarkable. As a result, the breakdown voltage of the gate insulating film becomes extremely low. The relationship between the breakdown electric field strength and the taper angle is shown in Figure 5. This breakdown electric field strength is highly dependent on the taper angle; When it was set below, a large value of 6 MV/cm was obtained.
最後に金属、透明導電膜より成るゲート電極109をス
パッタ法、真空蒸着法により形成する。Finally, a gate electrode 109 made of metal or a transparent conductive film is formed by sputtering or vacuum evaporation.
この様に構成された薄膜トランジスタは、テーパー角を
60度以下にすることにより、ゲート絶縁膜の破壊電圧
を大きくでき、薄膜トランジスタの欠陥を低減できる。In the thin film transistor configured in this manner, by setting the taper angle to 60 degrees or less, the breakdown voltage of the gate insulating film can be increased, and defects in the thin film transistor can be reduced.
又基板の温度を加熱することなく、ゲート絶縁膜を形成
できるため、基板に熱115m係数の大きいガラス基板
を用いた場合、形成されたゲート絶縁膜とガラス基板の
熱膨張係数の差が問題となることがなく基板の反り、変
形、ゲート絶縁膜のひび割れ等は生じない。In addition, since the gate insulating film can be formed without heating the substrate, if a glass substrate with a high thermal coefficient of 115 m is used as the substrate, the difference in thermal expansion coefficient between the formed gate insulating film and the glass substrate will be a problem. There is no warping or deformation of the substrate, cracking of the gate insulating film, etc.
又、効率よく、反応ガスを分解し膜を形成するため試料
室310の壁面等にはほとんど膜が付着することがなく
、原理的にパーティクルの発生は少なく、ピンホールの
ないゲート絶縁膜が容易に得られる。In addition, since the reaction gas is efficiently decomposed and a film is formed, there is almost no film adhering to the walls of the sample chamber 310, and in principle, fewer particles are generated, making it easy to form a gate insulating film without pinholes. can be obtained.
更に、反応ガスを供給する前に、5xlO−’Torr
以下の高真空とし、膜の形成もto−”r。Furthermore, before supplying the reaction gas, 5xlO-'Torr
The following high vacuum was applied, and the film formation was also carried out to -''r.
rr台で形成するため、形成されたゲート絶縁膜中の不
純物が極めて少なく、その結果薄膜トランジスタの表面
電荷密度も熱CVD法の1/3〜1/10と小さな値と
なり、薄膜トランジスタの信頼性を大幅に向上できる。Since it is formed on an RR stage, there are extremely few impurities in the formed gate insulating film, and as a result, the surface charge density of the thin film transistor is 1/3 to 1/10 of the thermal CVD method, which greatly improves the reliability of the thin film transistor. can be improved.
本発明の薄膜トランジスタの特性を第4図に示す、横軸
はゲート電圧vo・、縦軸はドレイン電流IQの対数値
である。ドレイン電圧v■は4v、チャネル長チャネル
幅ともに10μmである。半導体層には多結晶シリコン
を用いその膜厚は200人、ゲート絶縁膜はS i O
2を用いてその膜厚は1500人である。破線は従来の
熱CVD法によりゲート絶縁膜を形成した薄膜トランジ
スタ、実線は本発明のECRプラズマCVDにより形成
した薄膜トランジスタである。第4図から明らかな様に
表面電荷密度が減少したため、ゲート電圧Ovでのドレ
イン電流Inが約4桁小さくなり、サブスレショルド領
域での立上りも急峻となり特性が向上している。この結
果液晶デイスプレィに応用した場合低電圧駆動が可能と
なり、コントラスト比の大きい高画質のデイスプレィが
実現できる。The characteristics of the thin film transistor of the present invention are shown in FIG. 4, where the horizontal axis is the gate voltage vo· and the vertical axis is the logarithm of the drain current IQ. The drain voltage v■ is 4V, and both the channel length and channel width are 10 μm. The semiconductor layer is made of polycrystalline silicon and its thickness is 200 mm, and the gate insulating film is SiO.
2, the film thickness is 1500 people. The broken line represents a thin film transistor whose gate insulating film was formed by the conventional thermal CVD method, and the solid line represents a thin film transistor formed by the ECR plasma CVD method of the present invention. As is clear from FIG. 4, since the surface charge density has decreased, the drain current In at the gate voltage Ov has become smaller by about four orders of magnitude, and the rise in the subthreshold region has become steeper, improving the characteristics. As a result, when applied to a liquid crystal display, low-voltage driving becomes possible, and a high-quality display with a large contrast ratio can be realized.
イメージセンサや3次元集積回路へ応用した場合、低電
圧駆動、低消費電力が実現できる。When applied to image sensors and three-dimensional integrated circuits, low voltage drive and low power consumption can be achieved.
本発明は次のようなすぐれた効果を有する。第1に、薄
膜トランジスタのゲート絶縁膜の破壊電圧が大きくなり
、欠陥の低減、信頼性が向上できる。The present invention has the following excellent effects. First, the breakdown voltage of the gate insulating film of the thin film transistor increases, reducing defects and improving reliability.
第2に、ゲート絶縁膜とガラス基板の熱膨張係数の差が
問題となることがなく、基板の反り、変形、ゲート絶縁
膜のひび割れ等の発生はなく、大面積にわたり欠陥の少
ない薄膜トランジスタを形成できる。Second, the difference in thermal expansion coefficient between the gate insulating film and the glass substrate does not become a problem, and there is no warping or deformation of the substrate, cracking of the gate insulating film, etc., and thin film transistors with few defects can be formed over a large area. can.
第3に、薄膜トランジスタの表面電荷密度が1×10−
會1゜m−’〜3X10−”cm−”と少なく、信頼性
を大幅に向上できる。Third, the surface charge density of the thin film transistor is 1×10−
The distance is as small as 1°m-' to 3X10-"cm-", and reliability can be greatly improved.
第4にECRプラズマCVD法は原理的にパーティクル
の発生が少なく、ピンホール等の欠陥のないゲート絶縁
膜が容易に得られ、薄膜トランジスタの低欠陥化が実現
できる。Fourthly, the ECR plasma CVD method generates few particles in principle, and a gate insulating film without defects such as pinholes can be easily obtained, making it possible to reduce the number of defects in thin film transistors.
第5に、薄膜トランジスタの電気特性が向上し、低電圧
駆動が可能で高コントラスト比の液晶デイスプレィが実
現できる。Fifth, the electrical characteristics of thin film transistors are improved, and a liquid crystal display that can be driven at low voltage and has a high contrast ratio can be realized.
以上のように、本発明の薄膜トランジスタは数多くの優
れた効果を有するものであり、その応用範囲は、デイス
プレィ用のアクティブマトリックス基板やその周辺回路
、イメージセンサ、3次元集積回路など多岐にわたる。As described above, the thin film transistor of the present invention has many excellent effects, and its application range is wide-ranging, including active matrix substrates for displays, peripheral circuits thereof, image sensors, and three-dimensional integrated circuits.
第1図(a)(b)は本発明の薄膜トランジス夕の製造
方法を示した断面図。
第2図(a)(b)は従来の薄膜トランジスタの構造を
示しくa)は上視図、 (b)は断面図。
第3図はECRプラズマCVD装置の概略図。
第4図は薄膜トランジスタの特性を示すグラフ。
第5図はゲート絶縁膜の破壊電界強度とテーパー角の関
係を示すグラフ。
101.201,301・・・絶縁基板102.202
・・・ソース電極
103.203・・・ドレイン電極
107.206・・・半導体層
105.204・・・ソース配線
106.205・・・ドレイン配線
108.207・・・第一絶縁膜
304・・・イオン流
109.208・・・ゲート電極
303・・・プラズマ室
305・・・磁気コイル
306.308・・・ガスライン
307・・・マイクロ波
309・・・真空排気
310・・・試料室
311・・・石英窓FIGS. 1(a) and 1(b) are cross-sectional views showing a method of manufacturing a thin film transistor of the present invention. FIGS. 2(a) and 2(b) show the structure of a conventional thin film transistor, in which a) is a top view and FIG. 2(b) is a cross-sectional view. FIG. 3 is a schematic diagram of an ECR plasma CVD apparatus. FIG. 4 is a graph showing the characteristics of thin film transistors. FIG. 5 is a graph showing the relationship between the breakdown electric field strength and the taper angle of the gate insulating film. 101.201,301...Insulating substrate 102.202
...Source electrode 103.203...Drain electrode 107.206...Semiconductor layer 105.204...Source wiring 106.205...Drain wiring 108.207...First insulating film 304...・Ion flow 109.208...Gate electrode 303...Plasma chamber 305...Magnetic coil 306.308...Gas line 307...Microwave 309...Evacuation 310...Sample chamber 311 ...quartz window
Claims (2)
、該ソース電極と該ドレイン電極を結ぶ半導体層と、該
半導体層を被覆するゲート絶縁膜と、該ゲート絶縁膜を
介して設けられたゲート電極を具備する薄膜トランジス
タにおいて、該ソース電極及び該ドレイン電極の断面形
状の該基板面とエッチング面の成す角度(以下テーパー
角と呼ぶ)が60度以下であることを特徴とする薄膜ト
ランジスタ。(1) A source electrode and a drain electrode, a semiconductor layer connecting the source electrode and the drain electrode, a gate insulating film covering the semiconductor layer, and a gate insulating film provided on a predetermined substrate. 1. A thin film transistor comprising a gate electrode, wherein the angle formed between the substrate surface and the etched surface of the cross-sectional shape of the source electrode and the drain electrode (hereinafter referred to as a taper angle) is 60 degrees or less.
マCVD法(以下ECRプラズマCVD法と呼ぶ)で形
成したことを特徴とする請求項1記載の薄膜トランジス
タ。(2) The thin film transistor according to claim 1, wherein the gate insulating film is formed by an electron cyclotron resonance plasma CVD method (hereinafter referred to as ECR plasma CVD method).
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63234021A JP2841381B2 (en) | 1988-09-19 | 1988-09-19 | Method for manufacturing thin film transistor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63234021A JP2841381B2 (en) | 1988-09-19 | 1988-09-19 | Method for manufacturing thin film transistor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0282579A true JPH0282579A (en) | 1990-03-23 |
| JP2841381B2 JP2841381B2 (en) | 1998-12-24 |
Family
ID=16964317
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63234021A Expired - Lifetime JP2841381B2 (en) | 1988-09-19 | 1988-09-19 | Method for manufacturing thin film transistor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2841381B2 (en) |
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5362660A (en) * | 1990-10-05 | 1994-11-08 | General Electric Company | Method of making a thin film transistor structure with improved source/drain contacts |
| US5637512A (en) * | 1990-11-16 | 1997-06-10 | Seiko Epson Corporation | Method for fabricating a thin film semiconductor device |
| GB2391386A (en) * | 2002-06-06 | 2004-02-04 | Nec Corp | Method for forming pattern of stacked film |
| JP2006093652A (en) * | 2004-09-20 | 2006-04-06 | Samsung Sdi Co Ltd | ORGANIC THIN FILM TRANSISTOR AND FLAT DISPLAY DEVICE HAVING THE SAME |
| US7303945B2 (en) | 2002-06-06 | 2007-12-04 | Nec Corporation | Method for forming pattern of stacked film and thin film transistor |
| CN100375243C (en) * | 1994-09-16 | 2008-03-12 | 株式会社半导体能源研究所 | Manufacturing method of thin film semiconductor device |
| JP2009117460A (en) * | 2007-11-02 | 2009-05-28 | Citizen Finetech Miyota Co Ltd | Semiconductor substrate manufacturing method using soq substrate, and semiconductor substrate |
| JP2013102140A (en) * | 2011-10-13 | 2013-05-23 | Semiconductor Energy Lab Co Ltd | Semiconductor device and semiconductor manufacturing method |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5929289A (en) * | 1982-08-12 | 1984-02-16 | セイコーエプソン株式会社 | Substrate for liquid crystal panel |
| JPS6271276A (en) * | 1985-09-24 | 1987-04-01 | Mitsubishi Electric Corp | Manufacture of thin film transistor |
-
1988
- 1988-09-19 JP JP63234021A patent/JP2841381B2/en not_active Expired - Lifetime
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5929289A (en) * | 1982-08-12 | 1984-02-16 | セイコーエプソン株式会社 | Substrate for liquid crystal panel |
| JPS6271276A (en) * | 1985-09-24 | 1987-04-01 | Mitsubishi Electric Corp | Manufacture of thin film transistor |
Cited By (12)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5362660A (en) * | 1990-10-05 | 1994-11-08 | General Electric Company | Method of making a thin film transistor structure with improved source/drain contacts |
| US5637512A (en) * | 1990-11-16 | 1997-06-10 | Seiko Epson Corporation | Method for fabricating a thin film semiconductor device |
| CN100375243C (en) * | 1994-09-16 | 2008-03-12 | 株式会社半导体能源研究所 | Manufacturing method of thin film semiconductor device |
| GB2391386A (en) * | 2002-06-06 | 2004-02-04 | Nec Corp | Method for forming pattern of stacked film |
| GB2391386B (en) * | 2002-06-06 | 2004-11-17 | Nec Corp | Method for forming pattern of stacked film |
| US6933241B2 (en) | 2002-06-06 | 2005-08-23 | Nec Corporation | Method for forming pattern of stacked film |
| US7303945B2 (en) | 2002-06-06 | 2007-12-04 | Nec Corporation | Method for forming pattern of stacked film and thin film transistor |
| US7317227B2 (en) | 2002-06-06 | 2008-01-08 | Nec Corporation | Method for forming pattern of stacked film |
| US7781837B2 (en) | 2002-06-06 | 2010-08-24 | Nec Corporation | Stacked film including a semiconductor film having a taper angle, and thin film transistor including the stacked film |
| JP2006093652A (en) * | 2004-09-20 | 2006-04-06 | Samsung Sdi Co Ltd | ORGANIC THIN FILM TRANSISTOR AND FLAT DISPLAY DEVICE HAVING THE SAME |
| JP2009117460A (en) * | 2007-11-02 | 2009-05-28 | Citizen Finetech Miyota Co Ltd | Semiconductor substrate manufacturing method using soq substrate, and semiconductor substrate |
| JP2013102140A (en) * | 2011-10-13 | 2013-05-23 | Semiconductor Energy Lab Co Ltd | Semiconductor device and semiconductor manufacturing method |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2841381B2 (en) | 1998-12-24 |
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