JPH0543792B2 - - Google Patents

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Publication number
JPH0543792B2
JPH0543792B2 JP2145067A JP14506790A JPH0543792B2 JP H0543792 B2 JPH0543792 B2 JP H0543792B2 JP 2145067 A JP2145067 A JP 2145067A JP 14506790 A JP14506790 A JP 14506790A JP H0543792 B2 JPH0543792 B2 JP H0543792B2
Authority
JP
Japan
Prior art keywords
magnetic field
film
substrate
electric field
space
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
JP2145067A
Other languages
Japanese (ja)
Other versions
JPH0317274A (en
Inventor
Takashi Inushima
Naoki Hirose
Mamoru Tashiro
Shunpei Yamazaki
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.)
Semiconductor Energy Laboratory Co Ltd
Original Assignee
Semiconductor Energy Laboratory Co Ltd
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 Semiconductor Energy Laboratory Co Ltd filed Critical Semiconductor Energy Laboratory Co Ltd
Priority to JP14506790A priority Critical patent/JPH0317274A/en
Publication of JPH0317274A publication Critical patent/JPH0317274A/en
Publication of JPH0543792B2 publication Critical patent/JPH0543792B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明はマイクロ波電を加えるとともに、外部
磁場を加え、それらの相互作用を用い、かつその
電界の最も大きい空間に被膜形成手段を設け、被
膜形成を行うための薄膜形成装置および形成方法
に関する。
[Detailed Description of the Invention] [Field of Application of the Invention] The present invention applies microwave electricity and an external magnetic field, uses their interaction, provides a film forming means in the space where the electric field is largest, and forms a film. The present invention relates to a thin film forming apparatus and a forming method.

〔従来の技術〕[Conventional technology]

従来、薄膜の形成手段としてECR(電子サイク
ロトロン共鳴)を用い、その発散磁場を利用して
この共鳴空間より「離れた位置」に基板を配設
し、そこでの被膜特にアモルフアス構造を有する
被膜を形成する方法が知られている。
Conventionally, ECR (Electron Cyclotron Resonance) has been used as a means of forming thin films, and the diverging magnetic field is used to place a substrate at a position ``remote'' from this resonant space, and forms a film there, especially a film with an amorphous structure. There are known ways to do this.

さらに一般的にはかかるECR CVD(化学気相
法)に加えて、反応性ガスを用いる被膜形成手段
として数種類知られており、それらは熱CVD、
加熱フイラメントCVD、化学輸送法、13.56MHz
の周波数を用いるプラズマCVD法、マイクロ波
のみを用いるプラズマCVD法が知られている。
特にECR CVD法は活性種を磁場によりピンチン
グし、高エネルギ化することにより電子エネルギ
を大きくし、効率よく気体をプラズマ化させてい
る。しかしプラズマ化させることにより、気体が
有する高エネルギにより基板の被形成面がスパツ
タ(損傷)を受けることを防ぐため、このECR
条件を満たした空間より「難れた位置」に基板を
配設し、高エネルギ条件下でのプラズマ状態を避
けたイオンシヤワー化した反応性気体を到達させ
ることにより被膜形成または異方性エツチングを
行つていた。
Furthermore, in addition to ECR CVD (chemical vapor deposition), there are several known film forming methods using reactive gases, including thermal CVD,
Heated filament CVD, chemical transport method, 13.56MHz
Plasma CVD methods that use a frequency of , and plasma CVD methods that use only microwaves are known.
In particular, the ECR CVD method pinches active species using a magnetic field to increase the energy, thereby increasing the electron energy and efficiently converting gas into plasma. However, by turning it into plasma, the ECR
Film formation or anisotropic etching is achieved by arranging the substrate in a ``difficult position'' from the space that satisfies the conditions and delivering reactive gas in the form of an ion shower that avoids the plasma state under high energy conditions. I was gone.

〔従来の問題点〕[Conventional problems]

しかしかかるシヤワー化した反応性気体を用い
た被膜形成方法では、その気体の種類により異方
性エツチングまたはアモルフアス構造の被膜形成
等のエツチングまたはデイポジツシヨンのいずれ
か一方のプロセスのみを採用したものであつた。
そのため、この場合の被形成面上にはアモルフア
ス構造の被膜が形成されやすく、結晶性特に多結
晶性または単結晶を有する被膜の形成はきわめて
困難であつた。加えて高いエネルギを用いること
により、初めて反応性気体の活性化または反応を
させ得る被膜形成も不可能であつた。
However, such film forming methods using showered reactive gases employ either anisotropic etching or deposition process, such as anisotropic etching or film formation with an amorphous structure, depending on the type of gas. .
Therefore, in this case, a coating having an amorphous structure is likely to be formed on the surface to be formed, and it is extremely difficult to form a coating having crystallinity, particularly polycrystalline or single crystal. In addition, by using high energy, it was also impossible to form a film that could activate or react reactive gases for the first time.

〔問題を解決すべき手段〕[Means to solve the problem]

本発明は被膜形成をその一部でエツチングをさ
せつつ被膜形成を行わんとするもので、好ましく
は少なくとも一部に結晶性を有する被膜を形成せ
んとするものである。この目的のため、マイクロ
波電力の電界強度が最も大きくなる領域に被形成
面を有する基板を配設する。さらにその領域で電
場・磁場相互作用を有せしめる。例えば、ECR
(電子サイクロトロン共鳴)を生ぜしめる。さら
に磁場の強度程度を調整すると、この領域におい
てのみ初めて分解または反応をさせることができ
る被膜形成が可能となる。例えば、i−カーボン
(ダイヤモンドまたは微結晶粒を有する炭素被膜)
また高融点の金属またはセラミツク性絶縁被膜で
ある。
The present invention attempts to form a film while etching a part of the film, and preferably forms a film having crystallinity in at least a part of the film. For this purpose, a substrate having a surface to be formed is disposed in a region where the electric field strength of microwave power is greatest. Furthermore, electric field/magnetic field interaction is created in that region. For example, ECR
(electron cyclotron resonance). Furthermore, by adjusting the strength of the magnetic field, it becomes possible to form a film that can undergo decomposition or reaction only in this region. For example, i-carbon (diamond or carbon coating with microcrystalline grains)
It is also a high melting point metal or ceramic insulating coating.

すなわち本発明は従来より知られたマイクロ波
を用いたプラズマCVD法に磁場の力を加え、さ
らにマイクロ波の電場と磁場との相互作用、好ま
しくはECR(エレクトロンサイクロトロン共鳴)
条件又はホイツスラー共鳴条件を含む相互作用を
利用して、幅広い圧力範囲において高密度高エネ
ルギのプラズマを発生させる。その共鳴空間での
高エネルギ状態を利用して、例えば活性炭素原子
を多量に発生させ、再現性にすぐれ、均一な膜
厚、均質な特性のダイヤモンド、i−カーボン膜
等の被膜の形成を可能としたものである。また加
える磁場の強さを任意に変更可能な為、電子のみ
ではなく特定のイオンのECR条件を設定するこ
とができる特徴がある。
That is, the present invention adds the force of a magnetic field to the conventionally known plasma CVD method using microwaves, and further applies the interaction between the electric field of the microwave and the magnetic field, preferably ECR (electron cyclotron resonance).
Conditions or interactions involving Heutzler resonance conditions are used to generate dense, high-energy plasmas over a wide range of pressures. Utilizing the high energy state in the resonance space, it is possible to generate a large amount of activated carbon atoms and form films such as diamond and i-carbon films with excellent reproducibility, uniform thickness, and homogeneous properties. That is. Additionally, since the strength of the applied magnetic field can be changed arbitrarily, it is possible to set ECR conditions not only for electrons but also for specific ions.

また本発明の構成に付加して、マイクロ波と磁
場との相互作用により高密度プラズマを発生させ
た後、基板表面上まで至る間に高エネルギを持つ
光(例えば紫外光)を照射し、活性種にエネルギ
を与えつづけると、高密度プラズマ発生領域より
十分離れた位置においても高エネルギ状態に励起
された炭素原子が存在し、より大面積にダイヤモ
ンド、i−カーボン膜を形成することも可能であ
つた。
Additionally, in addition to the structure of the present invention, after high-density plasma is generated by the interaction of microwaves and a magnetic field, high-energy light (for example, ultraviolet light) is irradiated while reaching the substrate surface to activate the plasma. If energy is continued to be applied to the seeds, carbon atoms excited to a high energy state will exist even at a location sufficiently far from the high-density plasma generation region, making it possible to form a diamond or i-carbon film over a larger area. It was hot.

さらに磁場とマイクロ波の相互作用により発生
する高エネルギ励起種に直流バイアス電圧を加え
て、基板側に多量の励起子が到達するようにする
ことは薄膜の形成速度を向上させる効果があつ
た。
Furthermore, applying a DC bias voltage to the high-energy excited species generated by the interaction of the magnetic field and microwaves, so that a large number of excitons reached the substrate side, had the effect of increasing the rate of thin film formation.

以下に実施例を示し、さらに本発明を説明す
る。
Examples will be shown below to further explain the present invention.

〔実施例〕〔Example〕

第1図に本発明にて用いた磁場印加可能なマイ
クロ波プラズマCVD装置を示す。
FIG. 1 shows a microwave plasma CVD apparatus capable of applying a magnetic field used in the present invention.

同図において、この装置は減圧状態に保持可能
なプラズマ発生空間1、加熱空間3、補助空間
2、磁場を発生する電磁石5,5′およびその電
源25、マイクロ波発振器4、排気系を構成する
ターボ分子ポンプ8、ロータリーポンプ14、圧
力調整バルブ11、赤外線加熱ヒータ20、およ
びその電源23、赤外線反射面21、基板ホルダ
20′、基板10、マイクロ波導入窓15、ガス
導入系6,7、水冷系18,18′より構成され
ている。
In the figure, this device comprises a plasma generation space 1 that can be maintained in a reduced pressure state, a heating space 3, an auxiliary space 2, electromagnets 5 and 5' that generate a magnetic field and their power source 25, a microwave oscillator 4, and an exhaust system. Turbo molecular pump 8, rotary pump 14, pressure adjustment valve 11, infrared heater 20 and its power source 23, infrared reflecting surface 21, substrate holder 20', substrate 10, microwave introduction window 15, gas introduction system 6, 7, It is composed of water cooling systems 18 and 18'.

まず薄膜形成用基板10を基板ホルダ10′上
に設置する。このホルダは高熱伝導性を有し、か
つマイクロ波をできるだけ乱さないため、セラミ
ツクの窒化アルミニユームを用いた。この基板ホ
ルダを赤外線ヒータ20より放物反射面21レン
ズ系22を用いて集光し加熱する。(例えば500
℃)次に水素6を10SCCMガス系7を通して高密
度プラズマ発生領域2へと導入し、外部より
2.45GGHzの周波数のマイクロ波を500Wの強さで
加える。さらに、磁場約2Kガウスを磁石5,
5′より印加し、高密度プラズマをプラズマ発生
空間1にて発生させる。この時プラズマ発生空間
1の圧力は0.1Paに保持されている。この高密度
プラズマ領域より高エネルギを持つ水素原子また
は電子が基板10上に到り、表面を洗浄にする。
さらにこの水素を中止し、ガス系7より炭化物気
体例えばアセチレン(C2H2)、メタン(CH4)を
活性化せしめる。そして高エネルギに励起された
炭素原子が生成され、約500℃加熱された基板1
0上に、この炭素原子が体積し、ダイヤモンド又
はi−カーボン膜が形成される。
First, the thin film forming substrate 10 is placed on the substrate holder 10'. This holder is made of ceramic aluminum nitride because it has high thermal conductivity and does not disturb microwaves as much as possible. This substrate holder is heated by condensing light from an infrared heater 20 using a parabolic reflecting surface 21 and a lens system 22. (e.g. 500
℃) Next, hydrogen 6 is introduced into the high-density plasma generation region 2 through the 10SCCM gas system 7, and then
Apply microwaves with a frequency of 2.45GGHz at an intensity of 500W. Furthermore, a magnetic field of approximately 2K Gauss is applied to the magnet 5,
5' to generate high-density plasma in the plasma generation space 1. At this time, the pressure in the plasma generation space 1 is maintained at 0.1 Pa. Hydrogen atoms or electrons with high energy reach the substrate 10 from this high-density plasma region and clean the surface.
Furthermore, this hydrogen supply is stopped, and carbide gases such as acetylene (C 2 H 2 ) and methane (CH 4 ) are activated from the gas system 7. Carbon atoms excited with high energy are generated and the substrate 1 is heated to approximately 500℃.
These carbon atoms accumulate on the 0, forming a diamond or i-carbon film.

第1図において、磁場は2つのリング状の磁石
5,5′を用いたヘルムホルツコイル方式を採用
した。さらに、4分割した空間30に対し電場・
磁場の強度を調べた結果を第2図に示す。
In FIG. 1, a Helmholtz coil system using two ring-shaped magnets 5 and 5' is used for the magnetic field. Furthermore, the electric field and
Figure 2 shows the results of examining the strength of the magnetic field.

第2図Aにおいて、横軸(X軸)は空間20の
横方向(反応性気体の放出方向)であり、縦軸
(R軸)は磁石の直径方向を示す。図面における
曲線は磁場の等電位面を示す。そしてその線に示
されている数字は磁石5が約2000ガウスの時に得
られる磁場の強さを示す。磁石5の強度を調整す
ると、電極・磁場の相互作用を有する空間100
(875±185ガウス)で大面積において磁場の強さ
を基板の被形成面の広い面積にわたつて概略均一
にさせることができる。図面は等磁場面を示し、
特に線26が875ガウスとなるECR(電子サイク
ロトロン共鳴)条件を生ずる等磁場面である。
In FIG. 2A, the horizontal axis (X-axis) is the horizontal direction of the space 20 (reactive gas release direction), and the vertical axis (R-axis) is the diametrical direction of the magnet. The curves in the drawings indicate equipotential surfaces of the magnetic field. The number shown on the line indicates the strength of the magnetic field obtained when the magnet 5 is about 2000 Gauss. By adjusting the strength of the magnet 5, a space 100 with interaction between the electrodes and the magnetic field is created.
(875±185 Gauss), it is possible to make the strength of the magnetic field approximately uniform over a large area of the formation surface of the substrate. The drawing shows an isomagnetic scene,
In particular, line 26 is an isomagnetic scene that produces ECR (electron cyclotron resonance) conditions of 875 Gauss.

さらにこの共鳴条件を生ずる空間100は第2
図Bに示す如く、電場が最大となる領域となるよ
うにしている。第2図Bの横軸は第2図Aと同じ
く反応性気体の流れる方向を示し、縦軸は電場
(電界強度)の強さを示す。
Furthermore, the space 100 that produces this resonance condition is the second
As shown in Figure B, the area is set so that the electric field is maximum. The horizontal axis of FIG. 2B indicates the flow direction of the reactive gas, as in FIG. 2A, and the vertical axis indicates the strength of the electric field (electric field strength).

すると電界領域100以外に領域100′も最大とな
る領域に該当する。しかしにここに対応する磁場
(第2図A)はきわめて等磁場面が多く存在して
いる。即ち領域1000には基板の被形成面の直径方
向(第2図Aにおける縦軸方向)での膜厚のばら
つきが大きくなり、26′の共鳴条件を満たす
ECR条件部分で良質の被膜ができるのみである。
結果として均一かつ均質な被膜を期待できない。
Then, in addition to the electric field area 100, the area 100' also corresponds to the area where the electric field becomes maximum. However, the magnetic field corresponding to this (Fig. 2A) has many isomagnetic scenes. In other words, in region 1000, there is a large variation in film thickness in the diametrical direction (vertical axis direction in FIG. 2A) of the surface on which the substrate is formed, and the resonance condition of 26' is satisfied.
A good quality film can only be formed under ECR conditions.
As a result, a uniform and homogeneous coating cannot be expected.

もちろんドーナツ型に作らんとする場合はそれ
でもよい。
Of course, if you want to make it into a donut shape, that's fine.

また領域100に対してその原点対称の反対の側
にも電場が最大であり、かつ磁場が広い領域にわ
たつて一定となる領域を有する。基板の加熱を行
う必要がない場合はかかる空間での被膜形成が有
効である。しかしマイクロ波の電場を乱すことな
く加熱を行う手段が得にくい。
Further, on the opposite side of the region 100 symmetrical to the origin, there is a region where the electric field is maximum and the magnetic field is constant over a wide region. When there is no need to heat the substrate, forming a film in such a space is effective. However, it is difficult to find a way to perform heating without disturbing the microwave electric field.

これらの結果、基板の出し入れの容易さ、加熱
の容易さを考慮し、均一な膜でありかつ均質な被
膜とするためには第2図Aの領域100が3つの領
域の中では最も工業的に量産性の優れた位置と推
定される。
As a result, area 100 in Fig. 2A is the most industrial of the three areas in order to obtain a uniform film and a homogeneous coating, taking into account the ease of putting in and taking out the substrate and the ease of heating. It is estimated that it is in an excellent position for mass production.

この結果、本発明では領域100に基板10を配
設すると、この基板が円形であつた場合、半径
100mmまで、好ましくは半径50mmまでの大きさで
均一、均質に被膜形成が可能となつた。
As a result, in the present invention, when the substrate 10 is disposed in the region 100, if this substrate is circular, the radius
It has become possible to uniformly and homogeneously form a film with a radius of up to 100 mm, preferably up to 50 mm.

さらに大面積とするには、例えばこの4倍の面
積において同じく均一な膜厚とするには周波数を
2.45GHzではなく1.225GHzとすればこの空間の直
径(第2図AのR方向)を2倍とすることができ
る。
To make the area even larger, for example, to achieve the same uniform film thickness over an area four times as large as this, the frequency should be increased.
If it is set to 1.225 GHz instead of 2.45 GHz, the diameter of this space (direction R in Figure 2 A) can be doubled.

第3図は第2図における基板10の位置におけ
る円形空間の磁場Aおよび電場Bの等磁場、等電
場の図面である。第3図Bより明らかなごとく、
電場は最大25KV/mにまで達せしめ得ることが
わかる。
FIG. 3 is a drawing of equal magnetic fields and equal electric fields of the magnetic field A and the electric field B in a circular space at the position of the substrate 10 in FIG. 2. FIG. As is clear from Figure 3B,
It can be seen that the electric field can reach up to 25KV/m.

また比較のために同条件下で磁場を印加せずに
薄膜形成を行つた。その時基板上に形成された薄
膜はグラフアイト膜であつた。
For comparison, a thin film was formed under the same conditions without applying a magnetic field. The thin film formed on the substrate at that time was a graphite film.

さらに本実施例と同条件下において基板温度を
650℃以上とした場合ダイヤモンド薄膜を形成す
ることが可能であつた。
Furthermore, under the same conditions as in this example, the substrate temperature was
It was possible to form a diamond thin film when the temperature was 650°C or higher.

本実施例にて形成された薄膜の電子線回析像を
とつたところアモルフアス特有のハローパターン
とともにダイヤモンドのスポツトがみられ、i−
カーボン膜となつていた。さらに基板温度を上げ
て形成してゆくにしたがい、ハローパターンが少
しづつ消えてゆき650℃以上でダイヤモンドとな
つた。
When an electron beam diffraction image of the thin film formed in this example was taken, diamond spots were observed along with a halo pattern peculiar to amorphous amorphous.
It had become a carbon film. As the substrate temperature was raised further, the halo pattern gradually disappeared and turned into a diamond at temperatures above 650°C.

また基板加熱温度を150℃未満とした場合、磁
場を加えてもi−カーボン膜を作成することはで
きなかつた。
Furthermore, when the substrate heating temperature was less than 150° C., it was not possible to form an i-carbon film even when a magnetic field was applied.

かかる方式において、基板上に炭化珪化物気体
(メチルシラン)を用い炭化珪素の多結晶膜を作
ることができる。アルミニユーム化物気体とアン
モニアとの反応により窒化アルミニユーム被膜を
作ることもできる。さらにタングステン、チタ
ン、モリブデンまたはそれらの珪化物の高融点導
体を作ることもできる。
In this method, a polycrystalline film of silicon carbide can be formed on a substrate using a silicon carbide gas (methylsilane). Aluminum nitride coatings can also be produced by reaction of aluminide gas with ammonia. Furthermore, high melting point conductors of tungsten, titanium, molybdenum or their silicides can also be made.

〔効果〕〔effect〕

本発明の構成を取ることにより、従来作製され
ていた結晶性を少なくとも一部に有する被膜の作
製条件より幅広い条件下にて作製可能であつた。
By employing the configuration of the present invention, it was possible to produce a film under a wider range of conditions than conventionally produced films having at least a portion of crystallinity.

また従来法に比べて大面積に均一な薄膜を形成
することが可能であつた。
Furthermore, it was possible to form a uniform thin film over a larger area than with conventional methods.

さらに作製された薄膜は引張、圧縮とも膜応力
をほとんど有さない良好な膜であつた。
Furthermore, the produced thin film was a good film with almost no film stress in either tension or compression.

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

第1図は本発明で用いる磁場・電場相互作用を
用いたマイクロ波CVD装置の概略を示す。第2
図はコンピユータシミユレイシヨンによる磁場お
よび電場特性を示す。第3図は電場・磁場相互作
用をさせた位置での磁場および電場の特性を示
す。 1……プラズマ発生空間、10,10′……基
板および基板ホルダ、4……マイクロ波発振器、
5,5′……外部磁場発生器、20……基板加熱
ヒータ、100……最大電場となる空間。
FIG. 1 schematically shows a microwave CVD apparatus using magnetic field/electric field interaction used in the present invention. Second
The figure shows the magnetic field and electric field characteristics by computer simulation. Figure 3 shows the characteristics of the magnetic field and electric field at a position where the electric field and magnetic field interact. 1... Plasma generation space, 10, 10'... Substrate and substrate holder, 4... Microwave oscillator,
5, 5'...External magnetic field generator, 20...Substrate heater, 100...Space with maximum electric field.

Claims (1)

【特許請求の範囲】[Claims] 1 減圧状態に保持されたプラズマ発生室、該発
生室を囲んで設けられた磁場発生手段、前記プラ
スマ発生室にマイクロ波を供給する手段を備えた
磁場及び電場の相互作用を利用して被膜を形成す
る方法であつて、前記プラズマ発生室に炭化物気
体を導入し、該気体に対して外部より磁界及びマ
イクロ波を加え、電子サイクロトロン共鳴条件を
満たす共鳴磁場の±21.2%以内の磁場領域内に被
形成面を有する基板を設けることにより、被形成
面上にダイヤモンド膜を形成することを特徴とす
る被膜形成方法。
1. A plasma generation chamber maintained in a reduced pressure state, a magnetic field generation means provided surrounding the generation chamber, and a means for supplying microwaves to the plasma generation chamber. The coating is formed using the interaction of the magnetic field and electric field. In this method, a carbide gas is introduced into the plasma generation chamber, a magnetic field and microwaves are applied to the gas from the outside, and a magnetic field region within ±21.2% of a resonant magnetic field that satisfies electron cyclotron resonance conditions is provided. A method for forming a film, comprising: providing a substrate having a surface to be formed, and forming a diamond film on the surface to be formed.
JP14506790A 1990-06-01 1990-06-01 Film formation Granted JPH0317274A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14506790A JPH0317274A (en) 1990-06-01 1990-06-01 Film formation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14506790A JPH0317274A (en) 1990-06-01 1990-06-01 Film formation

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP61266834A Division JPS63121667A (en) 1986-11-10 1986-11-10 Device and method for forming thin film

Related Child Applications (2)

Application Number Title Priority Date Filing Date
JP6145738A Division JP2769977B2 (en) 1994-06-06 1994-06-06 Plasma processing method
JP6145739A Division JP2739286B2 (en) 1994-06-06 1994-06-06 Plasma processing method

Publications (2)

Publication Number Publication Date
JPH0317274A JPH0317274A (en) 1991-01-25
JPH0543792B2 true JPH0543792B2 (en) 1993-07-02

Family

ID=15376617

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14506790A Granted JPH0317274A (en) 1990-06-01 1990-06-01 Film formation

Country Status (1)

Country Link
JP (1) JPH0317274A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2769977B2 (en) * 1994-06-06 1998-06-25 株式会社半導体エネルギー研究所 Plasma processing method
KR20040033796A (en) * 2002-10-16 2004-04-28 현대자동차주식회사 Nozzle of injector
JP4739836B2 (en) * 2005-07-07 2011-08-03 トヨタ自動車株式会社 Control device for spark ignition type cylinder injection type internal combustion engine

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60103098A (en) * 1983-11-04 1985-06-07 Kyocera Corp Manufacture of diamond film

Also Published As

Publication number Publication date
JPH0317274A (en) 1991-01-25

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