JPS6126597A - Method and device for forming thin film - Google Patents

Method and device for forming thin film

Info

Publication number
JPS6126597A
JPS6126597A JP14731584A JP14731584A JPS6126597A JP S6126597 A JPS6126597 A JP S6126597A JP 14731584 A JP14731584 A JP 14731584A JP 14731584 A JP14731584 A JP 14731584A JP S6126597 A JPS6126597 A JP S6126597A
Authority
JP
Japan
Prior art keywords
substrate
thin film
plasma
magnetic field
vacuum chamber
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
JP14731584A
Other languages
Japanese (ja)
Inventor
Tadashi Serikawa
正 芹川
Shiro Suyama
陶山 史郎
Akio Okamoto
章雄 岡本
Seiichi Shirai
白井 誠一
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.)
NTT Inc
Original Assignee
Nippon Telegraph and Telephone 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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP14731584A priority Critical patent/JPS6126597A/en
Publication of JPS6126597A publication Critical patent/JPS6126597A/en
Pending legal-status Critical Current

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Classifications

    • C—CHEMISTRY; METALLURGY
    • C30—CRYSTAL GROWTH
    • C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B25/00—Single-crystal growth by chemical reaction of reactive gases, e.g. chemical vapour-deposition growth

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  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • General Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Crystals, And After-Treatments Of Crystals (AREA)

Abstract

PURPOSE:To obtain a thin film having improved physical properties in a high deposition speed, by impressing a magnetic field having a component in the direction along the plate face of a substrate on which a thin film is formed, generating a gas discharge in a zone in the vicinity of the substrate. CONSTITUTION:The vacuum tank 21, the electrode 22, the gas inlet 24, the heater 26, and the magnet 25 to provide a magnetic field having a component in the direction along the plate face of the substrate 23 are set. The substrate 23 is placed on the electrode 22, a gas at a given pressure is introduced from the gas inlet 24, and the substrate is heated by the heater 26, etc. In this state, when negative voltage or high-frequency voltage is impressed to the electrode 22, discharge is started to generate the plasma 27. The plasma 27 exists locally in the vicinity of the substrate surface due to magnetic field, especially in the zone 28 wherein a magnetic field parallel to the plate face of the substrate exists, and does not extend in the whole vacuum tank. By this localization of the plasma, a high electric current value is obtained even by lowering the voltage between the substrate and the plasma, a formation speed of thin film can be extremely enlarged, and a value >=1,000Angstrom /min is easily obtained.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、高堆積速度で薄膜の形成を行うことのできる
薄膜の形成方法ならびに薄膜の形成装置に係シ、特に真
空槽内でプラズマを発生させて薄膜形成を行うものであ
シ、利用分野は主として半導体装置の製造に適用するも
のである。
Detailed Description of the Invention [Field of Industrial Application] The present invention relates to a thin film forming method and a thin film forming apparatus capable of forming a thin film at a high deposition rate. It is used to form a thin film by generating heat, and its field of use is mainly in the manufacture of semiconductor devices.

〔従来の技術〕[Conventional technology]

半導体素子等を構成している薄膜の形成には、真空蒸着
法や気相成長法が広く用いられている。
Vacuum deposition methods and vapor phase growth methods are widely used to form thin films constituting semiconductor devices and the like.

特に後者の気相成長法では、薄膜の源と々る元素を気体
状態で供給できる。このために、真空蒸着法では困難な
薄膜を容易に形成できる利点がある。
In particular, in the latter vapor phase growth method, the elements that form the source of the thin film can be supplied in a gaseous state. For this reason, there is an advantage that thin films, which are difficult to form using vacuum evaporation methods, can be easily formed.

しかしながら、通常の気相成長法(CVD法)では、薄
膜の形成に要する基板の温度が著しく高く、この結果、
この方法の適用領域が極く狭い範囲に限定されているの
が実状である。基板温度が高いという問題は、基板の温
度を高める代シに、薄膜を形成するに必要な気体を供給
した状態で、プラズマを励起することによシ解決された
。この方法は、プラズマを用いる理由から、プラズマ気
相成長法(プラズマCVD法)と呼ばれている。しか、
早i通常のCVD法に比較して、低基板温度で薄膜の形
成は行えるが、種々の問題点も残されている。
However, in the normal vapor phase growth method (CVD method), the temperature of the substrate required to form a thin film is extremely high, and as a result,
The reality is that the application area of this method is limited to an extremely narrow range. The problem of high substrate temperature was solved by exciting the plasma while supplying the gas necessary to form the thin film instead of raising the temperature of the substrate. This method is called a plasma vapor deposition method (plasma CVD method) because it uses plasma. deer,
Although thin films can be formed at lower substrate temperatures than conventional CVD methods, various problems remain.

以下に、半導体素子において極めて重要な位置を占めて
いる窒化シリコン膜を例にとシ、プラズマCVD法の原
理を述べる。第1図は、広く用いられているプラズマC
VD装置の概略図である。真空槽11の内部の電極12
上に基板15を置いた後、真空槽に設けたガス導入口1
4から、薄膜を構成する元素を含むガス、この場合、S
iH4とNH,もしくはN2との混合ガスを、数十Pa
乃至数100Paの範囲の圧力まで導入する。さらに、
ヒータ15等により基板を加熱した状態で、電極12に
負電圧もしくは高周波電圧を印加し、プラズマ16を発
生する。
The principle of the plasma CVD method will be described below, taking as an example a silicon nitride film that occupies an extremely important position in semiconductor devices. Figure 1 shows the widely used plasma C
It is a schematic diagram of a VD device. Electrode 12 inside vacuum chamber 11
After placing the substrate 15 on top, the gas inlet 1 provided in the vacuum chamber
4, the gas containing the elements constituting the thin film, in this case S
A mixed gas of iH4 and NH or N2 is heated to several tens of Pa.
A pressure ranging from 100 Pa to several 100 Pa is introduced. moreover,
With the substrate heated by the heater 15 or the like, a negative voltage or high frequency voltage is applied to the electrode 12 to generate plasma 16.

このプラズマによ#) 、SiH4,NHBやN、の分
解、それらの分子や原子のイオン化・励起が促進され、
300℃乃至500℃の比較的低い基板温度で、窒化シ
リコン膜が形成される。
This plasma promotes the decomposition of SiH4, NHB and N, and the ionization and excitation of their molecules and atoms.
A silicon nitride film is formed at a relatively low substrate temperature of 300°C to 500°C.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかし、上記従来゛からの方法では、第1図に示したよ
うに、プラズマが基板表面近傍だけでなく、真空槽全体
にわたって生成される。この結果、幾つかの重要な問題
点が生じてくる。
However, in the conventional method described above, as shown in FIG. 1, plasma is generated not only near the substrate surface but also throughout the vacuum chamber. This results in several important problems.

従来法における問題点の一つとして、薄膜の形成速度が
小さく、数千1乃至数百27分の範囲にとどまることで
ある。この原因は、プラズマが真空槽に一様に拡が9、
基板へ流入する電流値が小さいからである。一方、形成
速度を大きくするには、この電流値を高めなければなら
ないが、これを行うと、プラズマと基板との間の電圧の
上昇がもたらされ、−皮形成した薄膜がスパッタ・エツ
チングされてくる。上述の理由から、従来からの方法で
はすでに述べたように形成速度に上限があった。さらに
、従来法における他の問題点は、真空槽の内壁上にも薄
膜が形成されることである。
One of the problems with the conventional method is that the thin film formation rate is slow and remains in the range of several thousand one to several hundred twenty-seven minutes. The reason for this is that the plasma spreads uniformly in the vacuum chamber9.
This is because the current value flowing into the substrate is small. On the other hand, to increase the formation rate, the value of this current must be increased, which leads to an increase in the voltage between the plasma and the substrate, which - sputter-etches the formed thin film. It's coming. For the reasons mentioned above, conventional methods have had an upper limit on the formation rate as previously mentioned. Furthermore, another problem with the conventional method is that a thin film is also formed on the inner wall of the vacuum chamber.

そして、真空槽内壁上に形成された薄膜が膜形成時に剥
離すると、プラズマを不安定にしたシ、基板上の薄膜の
特性を損う。このために、真空槽内壁の清掃を十分に行
わなければ、すぐれた特性の薄膜を得ることは困難とな
る。
If the thin film formed on the inner wall of the vacuum chamber peels off during film formation, it will make the plasma unstable and impair the properties of the thin film on the substrate. For this reason, it is difficult to obtain a thin film with excellent properties unless the inner wall of the vacuum chamber is thoroughly cleaned.

前述した実施例では、無機ガスを用いた場合について説
明したが、メタyやエタン等の有機ガスを含むガスを導
入して放電を起すと、有機物力1ら成る薄膜が重合形成
される。この方法は、無機物の場合と区別する目的から
、プラズマ重合法と呼ばれることもある。このプラズマ
重合も、第1図に示すものと、本質的に類似の装置を用
いて行れる。この場合も、無機物の時と同様、薄膜の形
成速度が小さく、さらに、真空槽内壁にも薄膜が形成す
る欠点がある。
In the above-mentioned embodiments, the case where an inorganic gas is used has been described, but when a gas containing an organic gas such as meta-y or ethane is introduced and a discharge is caused, a thin film made of organic material 1 is polymerized and formed. This method is sometimes called a plasma polymerization method to distinguish it from the case of inorganic materials. This plasma polymerization can also be carried out using equipment essentially similar to that shown in FIG. In this case as well, as in the case of inorganic materials, there is a drawback that the thin film formation rate is slow and a thin film is also formed on the inner wall of the vacuum chamber.

以上に述べたように、従来からの方法では、薄膜を用い
て構成されている半導体等の素子を製作する費用が高価
となった月製作された素子の製造歩留シや信頼性の低下
をきたす欠点があった。
As mentioned above, conventional methods have been known to reduce the manufacturing yield and reliability of devices manufactured using thin films due to the high cost of manufacturing them. There were some drawbacks.

〔問題点を解決するための手段〕 本発明はこれらの欠点を除去するために、薄膜を形成す
べき基板の板面に溢う方向の成分を有する磁界を印加し
た状態で、基板の近傍領域において、ガスの放電を生ぜ
しめる。以下に本発明の実施例を示して詳細に説明する
。
[Means for Solving the Problems] In order to eliminate these drawbacks, the present invention applies a magnetic field having a component in a direction overflowing to the surface of the substrate on which a thin film is to be formed, and then , causing a discharge of gas. Examples of the present invention will be shown and explained in detail below.

〔実施例〕〔Example〕

本発明の実施例を第2図に示す。第1図に示した従来か
らの装置と同様に、真空槽21.電極22゜ガス導入口
24.ヒータ26を有している。 しかし、従来からの
ものと異なり1基板25の板面に溢う成分の磁界を与え
る磁石25が新たに設置されている。
An embodiment of the invention is shown in FIG. Similar to the conventional apparatus shown in FIG. Electrode 22° Gas inlet 24. It has a heater 26. However, unlike the conventional one, a magnet 25 is newly installed to provide a magnetic field with a component that overflows the surface of one substrate 25.

このような装置に、基板23を電極22上に配し、所定
のガスを所望の圧力でガス導入口24から導入した後、
ヒータ吟26によシ基板を加熱する。
After placing the substrate 23 on the electrode 22 in such an apparatus and introducing a predetermined gas at a desired pressure from the gas inlet 24,
The substrate is heated by the heater 26.

なお、基板の加熱はガス導入前に行なっても良い。Note that the substrate may be heated before the gas is introduced.

この状態で、電極22に負電圧もしくは高周波電圧を印
加すると、放電が開始しプラズマ27が発生することは
、従来からのものと同じである。しかし、このプラズマ
27は磁界のために、基板表面近傍、特に、基板の板面
に平行な磁界の存在する領域2Bに局在し、真空槽全体
に拡がることはない。このプラズマの局在化により、基
板−プラズマ間の電圧を低くしても高電流値が得られ、
薄膜の形成速度が、従来法よシも著しく大きく出来、1
ooo;7tr。
In this state, when a negative voltage or a high frequency voltage is applied to the electrode 22, discharge starts and plasma 27 is generated, as in the conventional case. However, due to the magnetic field, this plasma 27 is localized near the substrate surface, particularly in the region 2B where the magnetic field parallel to the plate surface of the substrate exists, and does not spread throughout the vacuum chamber. Due to this localization of the plasma, a high current value can be obtained even if the voltage between the substrate and the plasma is low.
The thin film formation speed is significantly higher than that of the conventional method, and 1
ooo;7tr.

以上の値を得ることも容易である。さらに、プラズマが
真空槽全体に分布しないため、真空槽内壁への薄膜の形
成が阻止される。この結果、真空槽内壁からの薄膜の剥
離が軽減でき、プラズマの安定性ならびに膜特性を向上
できる。また、外部から磁界を印加すると、ガス圧を、
従来からのものよシ低くしても、プラズマは安定に発生
する。このために、薄膜の形成条件の設定が容易となる
と同時に、薄膜の形成に寄与せずに排気されてしまうガ
ス量を少なくできる。
Obtaining the above values is also easy. Furthermore, since the plasma is not distributed throughout the vacuum chamber, formation of a thin film on the inner wall of the vacuum chamber is prevented. As a result, peeling of the thin film from the inner wall of the vacuum chamber can be reduced, and plasma stability and film properties can be improved. In addition, when a magnetic field is applied externally, the gas pressure is
Plasma is generated stably even at lower temperatures than conventional ones. Therefore, it becomes easy to set the conditions for forming the thin film, and at the same time, the amount of gas that is exhausted without contributing to the formation of the thin film can be reduced.

本発明において本質的な役割を果している磁界の強さは
数十ガウス以上必要である。さらに、第2図に示した実
施例では、磁界の強度の安定化の目的で、ポールピース
29を置くことが有効である。
The strength of the magnetic field, which plays an essential role in the present invention, is required to be several tens of Gauss or more. Furthermore, in the embodiment shown in FIG. 2, it is effective to place a pole piece 29 for the purpose of stabilizing the strength of the magnetic field.

また、本発明は、有機・無機を問わず、極めて広範囲の
材料の薄膜の形成に適することは、前述の説明から明ら
かである。
Further, it is clear from the above description that the present invention is suitable for forming thin films of an extremely wide range of materials, regardless of whether they are organic or inorganic.

第3図は、本発明の他の実施例の一部を示すものであシ
、薄膜形成のよシ一層の均一化を目的としている。基板
31.電極32.磁石33.およびポールピース34か
ら成る。基板の板面に平行な方向の磁界が存在する領域
35においては特に高形成速度で薄膜が得られる。しか
し、基板を磁界に対して横切る方向、すなわち、図中の
矢印36の方向に相対的に移動させることにょシ、基板
上での均一化が図れ、本発明がよシ有効に実施される。
FIG. 3 shows a part of another embodiment of the present invention, which is aimed at making thin film formation more uniform. Substrate 31. Electrode 32. Magnet 33. and a pole piece 34. A thin film can be obtained at a particularly high formation rate in the region 35 where a magnetic field exists in a direction parallel to the surface of the substrate. However, by moving the substrate relative to the direction transverse to the magnetic field, that is, in the direction of arrow 36 in the figure, uniformity on the substrate can be achieved and the present invention can be more effectively implemented.

なお、このような運動を行うことにょシ、第2図を用い
て説明した本発明の利点が損われることはない。
Incidentally, even if such an exercise is performed, the advantages of the present invention explained using FIG. 2 will not be impaired.

ここで参考として従来例と同様な窒化シリコン膜の形成
を例にして本発明の実施例における典型的な条件を比較
すると、基板加熱温度はほぼ同じで600〜500℃程
度、印加する負電圧もしくは高周波電圧は従来のプラズ
マCVDと同程度あるいはかなシ少なくしても良く、印
加する磁界強度は数十ガウス〜1K ガウス程度、ガス
圧は従来よシ10〜100オーダ低くても良い。ガス圧
を、このように低くしてもプラズマが安定して発生する
ので、窒化シリコン膜の形成にあたシ従来よシ広範囲に
ガス圧力を選定することが可能となシ、薄膜の形成条件
の設定が容易となる。それによシ窒化シリコン膜の密度
等を広範囲に変えることが可能になる。
Here, for reference, when we compare the typical conditions in the embodiment of the present invention using the formation of a silicon nitride film similar to the conventional example, we find that the substrate heating temperature is almost the same, about 600 to 500 °C, and the applied negative voltage or The high frequency voltage may be on the same level as in conventional plasma CVD or may be lower, the applied magnetic field strength may be on the order of several tens of Gauss to 1K Gauss, and the gas pressure may be on the order of 10 to 100 lower than in the conventional plasma CVD. Plasma is generated stably even at such a low gas pressure, so when forming a silicon nitride film, it is possible to select a gas pressure from a wider range than before, and the thin film formation conditions The settings become easier. This makes it possible to vary the density, etc. of the silicon nitride film over a wide range.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれば良質な薄膜が高形
成速度で得られるために、これを用いる素子を安価にで
き、さらに、素子の製造歩留シや信頼性を向上できる利
点を本発明は有している。
As explained above, according to the present invention, since a high-quality thin film can be obtained at a high formation rate, devices using the same can be made at low cost, and furthermore, the manufacturing yield and reliability of the device can be improved. I have an invention.

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

第1図は従来からのプラズマCVD装置の断面図、第2
図は本発明装置の一実施例の断面図、第3図は、本発明
をさらに有効に実施するための構成の説明図。 11.21・・・真空槽、  12,22.32・・・
電極、  13,23.31・・・基板、  14.2
4・・・ガス導入口、  15.26・・・ヒータ。 16.27・・・プラズマ、  25.33・・・磁石
、28・・・基板の板面に平行な磁界の存在する領域(
プラズマが特に高密度となっている領域)、  29.
34・・・ポールピース、35・・・基板の板面に平行
な方向の磁界が存在する領域、36・・・矢印。
Figure 1 is a cross-sectional view of a conventional plasma CVD apparatus, Figure 2
The figure is a sectional view of one embodiment of the apparatus of the present invention, and FIG. 3 is an explanatory diagram of a configuration for implementing the present invention more effectively. 11.21...Vacuum chamber, 12,22.32...
Electrode, 13, 23.31... Substrate, 14.2
4...Gas inlet, 15.26...Heater. 16.27...Plasma, 25.33...Magnet, 28...A region where a magnetic field exists parallel to the plate surface of the substrate (
(regions where plasma is particularly dense), 29.
34...Pole piece, 35...A region where a magnetic field exists in a direction parallel to the plate surface of the substrate, 36...Arrow.

Claims (3)

【特許請求の範囲】[Claims] (1)真空槽内に、薄膜を堆積すべき基板を設置する工
程と、該薄膜を構成する元素を含むガスを前記真空槽内
に導入する工程と、該ガスを導入する工程の前または後
に前記薄膜を堆積すべき基板を加熱する工程と、前記基
板の板面に沿う方向の成分を有する磁界を与えた状態で
、前記真空槽内の前記基板の近傍領域において、前記ガ
スの放電を生ぜしめる工程とを含むことを特徴とする薄
膜の形成方法。
(1) A step of installing a substrate on which a thin film is to be deposited in a vacuum chamber, a step of introducing a gas containing an element constituting the thin film into the vacuum chamber, and before or after the step of introducing the gas. heating the substrate on which the thin film is to be deposited, and generating a discharge of the gas in a region near the substrate in the vacuum chamber while applying a magnetic field having a component in a direction along the plate surface of the substrate; A method for forming a thin film, comprising the step of tightening.
(2)真空槽と、該真空槽内に配置され薄膜を堆積する
基板を設置する支持体と、該薄膜を構成する元素を含む
ガスを前記真空槽内に導入する手段と、前記基板を加熱
する手段と、前記基板の板面に沿う方向の成分を有する
磁界を印加する手段と、負電圧もしくは高周波電圧を印
加する手段と、をそれぞれ具備し、前記真空槽内の前記
基板の近傍領域に、前記ガスの放電を生成させるように
構成することを特徴とする薄膜の形成装置。
(2) a vacuum chamber, a support placed in the vacuum chamber on which a substrate on which a thin film is deposited, a means for introducing a gas containing an element constituting the thin film into the vacuum chamber, and heating the substrate; means for applying a magnetic field having a component in a direction along the plate surface of the substrate, and means for applying a negative voltage or a high frequency voltage to a region near the substrate in the vacuum chamber. . A thin film forming apparatus, characterized in that it is configured to generate a discharge of the gas.
(3)真空槽と、該真空槽内に配置され薄膜を堆積する
基板を設置する支持体と、該薄膜を構成する元素を含む
ガスを前記真空槽内に導入する手段と、前記基板を加熱
する手段と、前記基板の板面に沿う方向の成分を有する
磁界を印加する手段と、負電圧もしくは高周波電圧を印
加する手段と、をそれぞれ具備し、前記真空槽内の前記
基板の近傍領域に、前記ガスの放電を生成させるように
構成し、さらに前記基板を、前記基板の板面に沿う方向
の成分を有する磁界に対して相対的に移動させる手段を
有することを特徴とする薄膜の形成装置。
(3) a vacuum chamber, a support placed in the vacuum chamber on which a substrate is deposited, a means for introducing a gas containing an element constituting the thin film into the vacuum chamber, and heating the substrate; means for applying a magnetic field having a component in a direction along the plate surface of the substrate, and means for applying a negative voltage or a high frequency voltage to a region near the substrate in the vacuum chamber. Formation of a thin film, characterized in that the method is configured to generate a discharge of the gas, and further includes means for moving the substrate relative to a magnetic field having a component in a direction along the plate surface of the substrate. Device.
JP14731584A 1984-07-16 1984-07-16 Method and device for forming thin film Pending JPS6126597A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14731584A JPS6126597A (en) 1984-07-16 1984-07-16 Method and device for forming thin film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14731584A JPS6126597A (en) 1984-07-16 1984-07-16 Method and device for forming thin film

Publications (1)

Publication Number Publication Date
JPS6126597A true JPS6126597A (en) 1986-02-05

Family

ID=15427408

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14731584A Pending JPS6126597A (en) 1984-07-16 1984-07-16 Method and device for forming thin film

Country Status (1)

Country Link
JP (1) JPS6126597A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5016564A (en) * 1986-12-29 1991-05-21 Sumitomo Metal Industries Ltd. Plasma apparatus
US5312778A (en) * 1989-10-03 1994-05-17 Applied Materials, Inc. Method for plasma processing using magnetically enhanced plasma chemical vapor deposition

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5756036A (en) * 1980-09-20 1982-04-03 Mitsubishi Electric Corp Plasma chemical vapor phase reactor
JPS60190562A (en) * 1984-03-08 1985-09-28 Tdk Corp Method and device for forming thin film

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5756036A (en) * 1980-09-20 1982-04-03 Mitsubishi Electric Corp Plasma chemical vapor phase reactor
JPS60190562A (en) * 1984-03-08 1985-09-28 Tdk Corp Method and device for forming thin film

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5016564A (en) * 1986-12-29 1991-05-21 Sumitomo Metal Industries Ltd. Plasma apparatus
US5019117A (en) * 1986-12-29 1991-05-28 Sumitomo Metal Industries Ltd. Plasma apparatus
US5312778A (en) * 1989-10-03 1994-05-17 Applied Materials, Inc. Method for plasma processing using magnetically enhanced plasma chemical vapor deposition

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