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JPS6315348B2 - - Google Patents
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JPS6315348B2 - - Google Patents

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Publication number
JPS6315348B2
JPS6315348B2 JP55032517A JP3251780A JPS6315348B2 JP S6315348 B2 JPS6315348 B2 JP S6315348B2 JP 55032517 A JP55032517 A JP 55032517A JP 3251780 A JP3251780 A JP 3251780A JP S6315348 B2 JPS6315348 B2 JP S6315348B2
Authority
JP
Japan
Prior art keywords
film
electric field
gas
forming
deposition 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.)
Expired
Application number
JP55032517A
Other languages
Japanese (ja)
Other versions
JPS56130465A (en
Inventor
Nobuo Kitajima
Tadaharu Fukuda
Juji Nishigaki
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP3251780A priority Critical patent/JPS56130465A/en
Publication of JPS56130465A publication Critical patent/JPS56130465A/en
Publication of JPS6315348B2 publication Critical patent/JPS6315348B2/ja
Granted legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/50Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating using electric discharges
    • C23C16/517Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating using electric discharges using a combination of discharges covered by two or more of groups C23C16/503 - C23C16/515

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • Plasma & Fusion (AREA)
  • General Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Physics & Mathematics (AREA)
  • Mechanical Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Photoreceptors In Electrophotography (AREA)
  • Chemical Vapour Deposition (AREA)
  • Light Receiving Elements (AREA)

Description

【発明の詳細な説明】 本発明は、グロー放電を利用して、例えば光導
電膜、半導体膜、無機絶縁膜或いは有機樹脂を形
成するに有効な膜形成法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a film forming method that is effective for forming, for example, a photoconductive film, a semiconductor film, an inorganic insulating film, or an organic resin using glow discharge.

膜形成用のガスを減圧にし得る堆積室内に導入
しグロー放電によるプラズマ現象を利用して所定
の支持体上に所望の特性を有する膜を形成しよう
とする場合、殊に、大面積の膜の場合には、全面
積に亘つてその膜厚並びに、電気的、光学的或い
は光電的等の物理特性の均一化及び品質の均一化
を計り乍ら、その膜形成速度を増大させることに
は、通常の真空蒸着法に較べて非常に困難が附纒
う。
When attempting to form a film with desired characteristics on a predetermined support by introducing a film-forming gas into a deposition chamber that can be under reduced pressure and utilizing the plasma phenomenon caused by glow discharge, it is especially important to form a film with desired characteristics on a given support. In some cases, increasing the film formation rate while ensuring uniformity of the film thickness, physical properties such as electrical, optical, or photoelectric properties, and uniformity of quality over the entire area, This method is much more difficult than the usual vacuum evaporation method.

例えば、SiH4ガスを放電エネルギーを使つて
分解し支持体上にアモルフアス水素化シリコン
(以後、a―Si:Hと記す)膜を形成して、この
膜の電気物性を利用し様とする場合、この膜の電
気特性が膜形成時の放電強度に大きく依存する
為、膜の全領域における電気物性の均一性を得る
には、膜形成の全領域において放電強度の均一化
を計る必要があり、この放電強度の均一化を計る
と共に、膜形成速度を向上させなければ再現性及
び生産性、量産性の点において充分満足され得る
ものではなく工業化を計ることは出来ない。
For example, when SiH 4 gas is decomposed using discharge energy to form an amorphous silicon hydride (hereinafter referred to as a-Si:H) film on a support, and the electrical properties of this film are to be utilized. Since the electrical properties of this film greatly depend on the discharge intensity during film formation, in order to obtain uniform electrical properties over the entire film area, it is necessary to equalize the discharge intensity over the entire film formation area. Unless the discharge intensity is made uniform and the film formation rate is improved, reproducibility, productivity, and mass production will not be fully satisfied, and industrialization will not be possible.

ところでこの放電強度の均一性は、電界強度、
ガス流量、ガス圧、ガスの導入位置と排出位置の
配置、放電電極の形状や配置等の要素に主に依存
し、従来より提案されている膜形成法では、上記
の諸要素を一義的に決定して、膜形成条件が最適
となる様な均一な放電強度を得ることは出来ず、
ある程度の条件緩和の下で膜形成を行なつている
のが現状である。
By the way, the uniformity of this discharge intensity is determined by the electric field strength,
It mainly depends on factors such as gas flow rate, gas pressure, arrangement of gas introduction and discharge positions, and the shape and arrangement of discharge electrodes, and conventionally proposed film formation methods do not uniquely address the above factors. It is not possible to obtain a uniform discharge intensity that optimizes the film formation conditions.
At present, film formation is performed under a certain degree of relaxed conditions.

殊に、電界強度は、形成される堆積膜の特性の
均一化に大いに影響を与えるものであるが、この
電界強度は、膜作成条件の他の要素に左右される
ことが大であつて、電界強度の不均一性、その強
度の経時的変化及び強度の大きさは、形成される
膜の特性に大きな影響を与える要因になつてい
る。例えば、従来より行なわれている放電用の電
界としては、直流電界又は高周波電界が利用され
ており、膜形成速度を上げる為に電界強度を高め
ることが試みられているが、直流電界法の場合に
は、高周波電界法に基づく実効的電界は強いが、
膜形成時のガス圧に強く依存し、低圧になるに従
つて、放電の低下、強いては放電停止を果たす。
又、逆に、ガス圧が高圧になるに従つて、放電を
形成する空間領域の中央寄りになるに従つて、電
界強度が急激に弱まり、低圧の場合と同様の現象
を引起して不都合である。
In particular, the electric field strength has a great influence on the uniformity of the properties of the deposited film that is formed, but this electric field strength largely depends on other factors in the film formation conditions. The non-uniformity of the electric field intensity, the change in the intensity over time, and the magnitude of the intensity are factors that greatly influence the characteristics of the formed film. For example, a direct current electric field or a high frequency electric field has been used as the electric field for conventional discharge, and attempts have been made to increase the electric field strength to increase the film formation rate, but in the case of the direct current electric field method, Although the effective electric field based on the high frequency electric field method is strong,
It strongly depends on the gas pressure during film formation, and as the pressure becomes lower, the discharge decreases and eventually stops.
Conversely, as the gas pressure becomes high, the electric field strength rapidly weakens as you move closer to the center of the spatial region where the discharge is formed, causing the same phenomenon as in the case of low pressure, which is inconvenient. be.

この様に、直流電界法においては、グロー放電
可能なガス圧の許容範囲が極めて狭く、又、ガス
圧の変動に大きく影響を受ける為に、均一特性の
膜を高速で作成するには不向きの面が多々存する
ものである。
As described above, in the DC electric field method, the allowable range of gas pressure that allows glow discharge is extremely narrow, and it is greatly affected by fluctuations in gas pressure, making it unsuitable for producing films with uniform characteristics at high speed. There are many aspects to it.

他方、高周波電界法の場合は、その放電は直流
電界法に比してガス圧の変動に対して安定性があ
り、この点においては、利点を有するが、直流電
界法に較べて実効電界強度が低く、従つて、膜形
成速度をそれ程高めることは出来ないという欠点
を有する。例えば、本発明者等の実験によれば、
精々7Å/sec程度である。従つて、例えばa―
Si:H膜等の極めて膜成長速度の小さい膜を作成
する場合には、膜作成に長時間を要し、生産性、
量産性には不向きである。
On the other hand, in the case of the high-frequency electric field method, the discharge is more stable against fluctuations in gas pressure than in the DC electric field method, and in this respect it has an advantage; It has the disadvantage that the film formation rate cannot be increased that much. For example, according to experiments conducted by the present inventors,
It is about 7 Å/sec at most. Therefore, for example, a-
When creating a film with an extremely low growth rate, such as a Si:H film, it takes a long time to create the film, which reduces productivity.
It is not suitable for mass production.

本発明は上記の諸点に鑑み成されたものであつ
て、大面積に亘つて均一特性の膜を高効率で製造
し得る膜形成法を提案することを目的とする。
The present invention has been made in view of the above points, and it is an object of the present invention to propose a film forming method capable of manufacturing a film with uniform characteristics over a large area with high efficiency.

本発明の膜形成法は、減圧にし得る堆積室内に
堆積膜形成用のガスを導入してグロー放電を生起
させて前記ガスのプラズマ雰囲気を形成して、前
記堆積室内に予め設置されてある膜形成用の支持
体上に堆積膜を形成する膜形成法において、前記
プラズマ雰囲気の形成を直流電場と交番電場の共
存下において行なう事を特徴とするものである。
この様な特徴を有する本発明の膜形成法によれば
従来法に較べて著しく高効率・高速度で物理的特
性、光学的特性及び光電的特性に優れ、然も形成
される膜の全領域においてそれ等の特性及び膜厚
が均一で且つ大面積のものが容易に形成し得るも
のである。殊に、本発明の膜形成法は、電気的及
び光電的に優れたa―Si:H膜が容易に再現性良
く高速度で形成し得るもので例えば、従来のグロ
ー放電法に較べ、少なくとも5〜10倍の膜形成速
度で光電的・電気的特性に優れたものが得られる
ものである。
In the film forming method of the present invention, a gas for forming a deposited film is introduced into a deposition chamber that can be reduced in pressure, a glow discharge is generated, and a plasma atmosphere of the gas is formed. A film forming method for forming a deposited film on a support for formation is characterized in that the plasma atmosphere is formed in the coexistence of a direct current electric field and an alternating electric field.
The film forming method of the present invention, which has these characteristics, has significantly higher efficiency and speed than conventional methods, has excellent physical properties, optical properties, and photoelectric properties, and can cover all areas of the formed film. In this case, those having uniform characteristics and film thickness and having a large area can be easily formed. In particular, the film forming method of the present invention can easily form an a-Si:H film with excellent electrical and photoelectric properties at high speed with good reproducibility, and for example, compared to the conventional glow discharge method, at least A film with excellent photoelectric and electrical properties can be obtained at a film formation rate 5 to 10 times faster.

本発明において交番電界としては好ましく採用
されるのは、交流電界であつて、電界の形成には
インダクテイブ法及びキヤパシテイブ法のいずれ
も採用し得る。
In the present invention, an alternating electric field is preferably employed as the alternating electric field, and either an inductive method or a capacitive method may be employed to form the electric field.

この様な交番電界の形成に要する電気エネルギ
ーとしては、インダクテイブ法の場合には、通常
は50W〜2KW、好適には100W〜1KWとされ、
キヤパシテイブ法の場合には、通常は、5W〜
500W、好適には10W〜100Wとされるのが望まし
いものである。
The electrical energy required to form such an alternating electric field is usually 50W to 2KW, preferably 100W to 1KW, in the case of the inductive method.
In the case of capacitive method, usually 5W~
It is desirable that the power is 500W, preferably 10W to 100W.

周波数としては、高い方が、本発明の目的を一
層効果的に達成され得るものであるが実用性の点
より、通常採用されているRF(radio frequency)
領域の周波数が好適に採用され、例えば13.56Mz
は好都合である。
Although the purpose of the present invention can be achieved more effectively with a higher frequency, from the point of view of practicality, the commonly used RF (radio frequency)
Frequencies in the region are preferably adopted, for example 13.56Mz
is convenient.

直流電界の形成に要する電気エネルギーとして
は、直流電界の形成に要する電極の電極間電位差
の絶対値が、通常0.1V〜1KV、好適には1V〜
500Vとされるのが望ましい。
As for the electrical energy required to form a DC electric field, the absolute value of the potential difference between the electrodes required to form a DC electric field is usually 0.1V to 1KV, preferably 1V to
It is desirable to set it to 500V.

本発明においては、堆積膜形成用の支持体は、
プラズマ雰囲気の形成されている空間領域の内或
いは何れの空間領域に設置されても良いものであ
るが、形成する堆積膜の種類によつて、より一層
高効率で膜形成が成され、且つ特性が均一で優れ
ている膜の得られる設置は決定される。
In the present invention, the support for forming a deposited film is
Although it may be installed in a spatial region where a plasma atmosphere is formed or in any spatial region, the film can be formed with higher efficiency and characteristics depending on the type of deposited film to be formed. The resulting placement of the membrane is determined to be uniform and excellent.

通常の場合、この支持体の設置位置は直流電界
を形成する電極の何れか一方の側とされ、好まし
くは、一方の電極に接触する位置、又はその近傍
の位置が選択される。
Normally, the support is installed on either side of the electrodes that form the DC electric field, and is preferably selected at a position in contact with one of the electrodes or in the vicinity thereof.

例えばa―Si:H膜を形成するのであれば、直
流電界形成用の電極の陰極側に設置される方が総
合的な観点より好ましいものである。
For example, if an a-Si:H film is to be formed, it is more preferable from a comprehensive viewpoint to install it on the cathode side of the electrode for forming a DC electric field.

以下、本発明を図面に従つて具体的に説明す
る。
The present invention will be specifically described below with reference to the drawings.

第1図は、本発明の膜形成法を具現化する堆積
装置の好適な例の1つを示す模式的説明図であ
る。第1図に示される堆積装置100は、堆積室
101の内部にプラズマを形成する為電界も形成
する為の電極107―1,107―2、RFコイ
ル110、及び電極107―1側に堆積膜形成用
の支持体109が各々設けてある。
FIG. 1 is a schematic explanatory diagram showing one preferred example of a deposition apparatus that embodies the film forming method of the present invention. The deposition apparatus 100 shown in FIG. 1 includes electrodes 107-1 and 107-2 for forming an electric field to form plasma inside a deposition chamber 101, an RF coil 110, and a deposited film on the electrode 107-1 side. A forming support 109 is provided in each case.

堆積室101には、該室101内を排気する為
の排気用パイプ112、堆積膜形成用のガスを導
入する為のガス導入パイプ106が接続されてい
る。電極107―1,107―2には、リード線
113―1,113―2を通じて外部にある直流
電源108より電圧が印加され、又、RFコイル
110にはリード線114を通じて外部のRF電
源111より所定の電力が投入される。第1図に
示す装置100によつて膜形成するには、先ず、
ガス流量調節バルブ104を閉じ、メインバルブ
103を全開して排気装置102によつて、堆積
室101内を排気して、所定の真空度にする。堆
積室101内が所望の真空度になつた時点で、必
要に応じて、支持体109を、適当な手段、例え
ばヒータ、赤外線ランプ等で所定の温度まで加熱
する。堆積室101内が、膜形成の為の準備が成
された時点において、3つのバルブ115―1,
115―2,115―3の中の所望のバルブを全
開しガス流量調節バルブ104を徐々に開いて、
所望のガスボンベ105より所望のガスを堆積室
101内に導入する。
The deposition chamber 101 is connected to an exhaust pipe 112 for exhausting the inside of the chamber 101, and a gas introduction pipe 106 for introducing gas for forming a deposited film. Voltage is applied to the electrodes 107-1, 107-2 from an external DC power source 108 through lead wires 113-1, 113-2, and voltage is applied to the RF coil 110 from an external RF power source 111 through a lead wire 114. A predetermined power is applied. To form a film using the apparatus 100 shown in FIG.
The gas flow rate control valve 104 is closed, the main valve 103 is fully opened, and the inside of the deposition chamber 101 is evacuated by the exhaust device 102 to achieve a predetermined degree of vacuum. When the desired degree of vacuum is achieved in the deposition chamber 101, the support 109 is heated to a predetermined temperature using an appropriate means such as a heater or an infrared lamp, if necessary. When the interior of the deposition chamber 101 is ready for film formation, three valves 115-1,
115-2, 115-3, and gradually open the gas flow rate adjustment valve 104.
A desired gas is introduced into the deposition chamber 101 from a desired gas cylinder 105 .

ガスの導入によつて、堆積室101内が所望の
真空度になつた時点で、電極107―1,107
―2間に所定の電位差が形成される様に、電極1
07に直流電源102より電圧を印加すると共
に、RF電源111よりRFコイル110に交番電
力を投入して、電極107―1,107―2内に
グロー放電を生起させて、堆積膜形成用のガスの
プラズマ雰囲気を形成する。プラズマ雰囲気の維
持は、好ましくは、膜形成終了まで連続的に持続
するのが均一特性の膜を形成するのに良いもので
ある。
When the desired degree of vacuum is reached in the deposition chamber 101 by introducing the gas, the electrodes 107-1, 107
- electrode 1 so that a predetermined potential difference is formed between the electrodes 1 and 2.
07 from the DC power supply 102, and alternating power is applied to the RF coil 110 from the RF power supply 111 to generate glow discharge in the electrodes 107-1 and 107-2. to form a plasma atmosphere. Preferably, the plasma atmosphere is maintained continuously until the end of film formation, in order to form a film with uniform characteristics.

電極107―1,107―2間の距離は、形成
する膜の種類、大きさ、堆積装置100の大きさ
等によつて任意に設定されるものであるが、例え
ば、a―Si:H膜を70cm角の平面積に形成するの
であれば3〜5cmの間に設定される。
The distance between the electrodes 107-1 and 107-2 can be arbitrarily set depending on the type and size of the film to be formed, the size of the deposition apparatus 100, etc. If it is to be formed on a 70 cm square plane area, it should be set between 3 and 5 cm.

次に、第1図に示されるのと同様の装置によつ
て、a―Si:H膜を形成した例を示す。
Next, an example will be shown in which an a-Si:H film was formed using an apparatus similar to that shown in FIG.

前述の様にして、堆積室101内の膜形成の準
備を計つた後、バルブ115―1,115―2を
混合比が9:1に成る様に開き、ガス流量調節バ
ルブ104を徐々に開いて、50SCCMの流量で
H2とSiH4の混合ガスを堆積室101に導入した。
この時、メインバルブ103の開閉量を調節して
堆積室101内の真空度が1〜10Torrの範囲に
なる様にした。
After preparing for film formation in the deposition chamber 101 as described above, the valves 115-1 and 115-2 are opened so that the mixing ratio becomes 9:1, and the gas flow rate control valve 104 is gradually opened. With a flow rate of 50SCCM
A mixed gas of H 2 and SiH 4 was introduced into the deposition chamber 101 .
At this time, the opening/closing amount of the main valve 103 was adjusted so that the degree of vacuum in the deposition chamber 101 was in the range of 1 to 10 Torr.

この時の装置各部の寸法、被処理材の寸法及び
材質は以下のようであつた。
At this time, the dimensions of each part of the apparatus and the dimensions and material of the material to be treated were as follows.

電極の寸法 120×120mm 電極間距離 50mm 被処理材の寸法 100×100mm 被処理材の材質 コーニング7059ガラス この状態で電源108をON状態にして電極1
07―1,107―2間に電位差50Vを形成し
た。又、RF電源111をON状態にしてRFコイ
ル110に13.56Mzで10Wの電力の投入を継続し
た。この場合、電極107―1,107―2間に
グロー放電が生起されてプラズマ雰囲気が形成さ
れ、支持体109上にa―Si:H膜が形成され
た。
Dimensions of electrode 120×120mm Distance between electrodes 50mm Dimensions of material to be treated 100×100mm Material of material to be treated Corning 7059 glass In this state, turn on power supply 108 and turn electrode 1
A potential difference of 50V was created between 07-1 and 107-2. Further, the RF power supply 111 was turned on and 10W of power at 13.56Mz was continuously applied to the RF coil 110. In this case, a glow discharge was generated between the electrodes 107-1 and 107-2, a plasma atmosphere was formed, and an a-Si:H film was formed on the support 109.

この時、膜厚が10μ迄は、略々30Å/secの堆積
速度で膜形成が成され、更に膜厚が50μになつて
も堆積速度は約20Å/secであり、極めて、高効
率・高速度でa―Si:H膜が形成されることが判
かつた。
At this time, the film is formed at a deposition rate of approximately 30 Å/sec up to a film thickness of 10 μm, and even when the film thickness reaches 50 μm, the deposition rate is approximately 20 Å/sec, making it extremely efficient and highly efficient. It was found that an a-Si:H film was formed at a high speed.

又、得られたa―Si:H膜は、全面積にわたり
その膜厚分布が5%以内である極めて均一な膜厚
を有していた。
Further, the obtained a-Si:H film had an extremely uniform film thickness with a film thickness distribution within 5% over the entire area.

さらに、その暗抵抗値は10-12Ωcm前後の値を
示し、室内光により数桁の抵抗値変化を示すな
ど、均一で良好な光導電体としての優れた特性を
有するものであつた。
Furthermore, the dark resistance value was around 10 -12 Ωcm, and the resistance value changed by several orders of magnitude with room light, indicating that it had excellent properties as a uniform and good photoconductor.

第2図は、電子写真感光体用の基体の様に円筒
状の膜形成用の支持体の上に膜形成する為の電極
の配置を示した模式的一部破断斜視図である。膜
形成用の円筒状支持体201は、直流電界形成用
の一方の電極も兼ねて、RFコイル202の内側
に、配置される。電極兼用支持体201と対向す
る直流電界形成用の他方の電極203は、RFコ
イル202の外側に図に示す様に配置される。
FIG. 2 is a schematic partially cutaway perspective view showing the arrangement of electrodes for forming a film on a cylindrical support for film formation, such as a substrate for an electrophotographic photoreceptor. A cylindrical support body 201 for film formation is placed inside the RF coil 202 and also serves as one electrode for forming a DC electric field. The other electrode 203 for forming a DC electric field, which faces the electrode-cum-support body 201, is arranged outside the RF coil 202 as shown in the figure.

堆積膜形成用のガスの堆積室内への導入は、第
2図の装置の場合、RFコイル202中を通つて、
RFコイル202に設けられた微細な孔である多
数のガス放出口204より成される。
In the case of the apparatus shown in FIG. 2, the gas for forming the deposited film is introduced into the deposition chamber through the RF coil 202.
It is made up of a large number of gas discharge ports 204, which are fine holes provided in the RF coil 202.

RFコイル202は、不図示のRF電源に結像さ
れ、又電極203、支持体201は、直流電界形
成用の電源(不図示)に各々電気的に接続されて
いる。この第2図の例の場合には、直流電界形成
用の一方の電極として膜形成用の支持体で兼用す
る為、電極の汚染、部品設置の為の空間的節約が
出来ると共に、RFコイル202を通じて膜形成
用のガスを堆積室内に導入するので、ガス分布の
一層の均一化を計ることが出来、極めて経済的且
つ量産的である。
The RF coil 202 is imaged by an RF power source (not shown), and the electrode 203 and the support 201 are each electrically connected to a power source (not shown) for forming a DC electric field. In the case of the example shown in FIG. 2, since the support for film formation also serves as one electrode for forming a DC electric field, it is possible to prevent contamination of the electrode and save space for installing parts, and the RF coil 202 Since the film-forming gas is introduced into the deposition chamber through the film, the gas distribution can be made even more uniform, making it extremely economical and suitable for mass production.

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

第1図は、本発明の膜形成法を具現化する堆積
装置の好適な例の1つを示す模式的説明図、第2
図は、他の例の1つを示す模式的一部破断斜視図
である。 100…堆積装置、101…堆積室、102…
排気装置、103…メインバルブ、104…ガス
流量調節バルブ、105…ガスボンベ、106…
ガス導入パイプ、107…電極、108…直流電
源、109…支持体、110…RFコイル、11
1…RF電源、112…排気パイプ、113,1
14…リード線、115…バルブ、201…円筒
状支持体、202…RFコイル、203…電極、
204…ガス放出口。
FIG. 1 is a schematic explanatory diagram showing one preferred example of a deposition apparatus embodying the film forming method of the present invention, and FIG.
The figure is a schematic partially cutaway perspective view showing one of the other examples. 100... Deposition device, 101... Deposition chamber, 102...
Exhaust device, 103... Main valve, 104... Gas flow rate adjustment valve, 105... Gas cylinder, 106...
Gas introduction pipe, 107... Electrode, 108... DC power supply, 109... Support body, 110... RF coil, 11
1...RF power supply, 112...exhaust pipe, 113,1
14... Lead wire, 115... Valve, 201... Cylindrical support, 202... RF coil, 203... Electrode,
204...Gas discharge port.

Claims (1)

【特許請求の範囲】[Claims] 1 減圧にし得る堆積室内に堆積膜形成用のガス
を導入してグロー放電を生起させて前記ガスのプ
ラズマ雰囲気を形成して、前記堆積室内に予め設
置されてある膜形成用の支持体上に堆積膜を形成
する膜形成法において、前記プラズマ雰囲気の形
成を直流電場と交番電場の共存下において行なう
事を特徴とする膜形成法。
1. A gas for forming a deposited film is introduced into a deposition chamber that can be reduced in pressure, and a glow discharge is generated to form a plasma atmosphere of the gas, and the gas is deposited on a support for forming a film that has been installed in advance in the deposition chamber. A film forming method for forming a deposited film, characterized in that the plasma atmosphere is formed under the coexistence of a direct current electric field and an alternating electric field.
JP3251780A 1980-03-14 1980-03-14 Film forming method Granted JPS56130465A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3251780A JPS56130465A (en) 1980-03-14 1980-03-14 Film forming method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3251780A JPS56130465A (en) 1980-03-14 1980-03-14 Film forming method

Publications (2)

Publication Number Publication Date
JPS56130465A JPS56130465A (en) 1981-10-13
JPS6315348B2 true JPS6315348B2 (en) 1988-04-04

Family

ID=12361153

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3251780A Granted JPS56130465A (en) 1980-03-14 1980-03-14 Film forming method

Country Status (1)

Country Link
JP (1) JPS56130465A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS571231A (en) * 1980-06-04 1982-01-06 Res Dev Corp Of Japan Plasma chemical vapour deposition cvd device
JPS58118111A (en) * 1982-01-07 1983-07-14 Ulvac Corp Plasma cvd apparatus
JPS5997514A (en) * 1982-11-22 1984-06-05 Agency Of Ind Science & Technol Solar cell manufacturing method
JPS6167923A (en) * 1984-09-12 1986-04-08 Fujitsu Ltd Plasma chemical vapor-phase growth

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5368171A (en) * 1976-11-30 1978-06-17 Hitachi Ltd Method and apparatus for plasma treatment
JPS6035059B2 (en) * 1977-12-22 1985-08-12 キヤノン株式会社 Electrophotographic photoreceptor and its manufacturing method
JPS5521515A (en) * 1978-07-31 1980-02-15 Oyo Kagaku Kenkyusho Surface treatment

Also Published As

Publication number Publication date
JPS56130465A (en) 1981-10-13

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