JPH0533812B2 - - Google Patents
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- Publication number
- JPH0533812B2 JPH0533812B2 JP62062666A JP6266687A JPH0533812B2 JP H0533812 B2 JPH0533812 B2 JP H0533812B2 JP 62062666 A JP62062666 A JP 62062666A JP 6266687 A JP6266687 A JP 6266687A JP H0533812 B2 JPH0533812 B2 JP H0533812B2
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- JP
- Japan
- Prior art keywords
- film
- plasma
- gas
- reaction
- electrode
- Prior art date
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Classifications
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/50—Photovoltaic [PV] energy
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- Photovoltaic Devices (AREA)
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は、光CVD法や励起された中性粒子に
よるCVD法を使用する成膜装置に関するもので
ある。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a film forming apparatus that uses a photo CVD method or a CVD method using excited neutral particles.
[従来の技術]
従来行われてきた光化学反応、例えば、シラン
ガスを主原料とするアモルフアスシリコンの光
CVD法においては、シランガスが波長160nm以
下の紫外線によつてしか直接光分解せず、また、
この波長の紫外線を放射する適切な光源が得にく
いため、水銀を触媒とする水銀増感光化学反応が
用いられてきた。しかし、この方法では触媒とし
て使用された水銀が膜中に混入し、これが悪影響
を及ぼす可能性があり、、さらには有毒である水
銀の管理上の問題点があつた。一方、ジシラン等
の高次シランを用いると、水銀増感反応を利用す
ることなく、低圧水銀灯等の光により直接光分解
が可能であり、水銀の悪影響は排除できるが、高
次シランは高価であり、その成膜速度も0.25Å/
秒程度であつて実用性から見てまだ不充分であ
る。[Conventional technology] Photochemical reactions that have been carried out in the past, such as the photochemical reaction of amorphous silicon whose main raw material is silane gas.
In the CVD method, silane gas is only directly photodecomposed by ultraviolet light with a wavelength of 160 nm or less;
Since it is difficult to obtain a suitable light source that emits ultraviolet light at this wavelength, mercury-sensitized photochemical reactions using mercury as a catalyst have been used. However, in this method, mercury used as a catalyst may be mixed into the membrane, which may have an adverse effect, and there are also problems in managing mercury, which is toxic. On the other hand, when higher-order silanes such as disilane are used, direct photolysis is possible using light from a low-pressure mercury lamp without using mercury sensitization, and the negative effects of mercury can be eliminated, but higher-order silanes are expensive. Yes, and the deposition rate is 0.25Å/
This is about seconds, which is still insufficient from a practical standpoint.
そして、13.56MHzの高周波放電によりシラン
を分解して堆積させる成膜方法が一般的に行われ
ているが、荷電粒子により堆積膜が損傷を受た
り、膜中に不純物が混入する問題点があつた。 A commonly used film formation method is to decompose and deposit silane using a high-frequency discharge of 13.56 MHz, but there are problems such as the deposited film being damaged by charged particles and impurities getting mixed into the film. Ta.
そこで、水銀の悪影響がなく、不純物や荷重粒
子損傷のない高品質で均一な薄膜を充分に速くて
実用化可能な堆積速度を可能とする成膜方法とし
て、プラズマから照射される紫外線を用いて光化
学反応を生起せしめ、プラズマと分離された基板
上に反応生成物を堆積して成膜することが行われ
る。この光CVD法に使用される成膜装置は、一
つの容器内に、ガス放電によつて形成されるプラ
ズマ領域と、膜形成を行う基板が配置され、化学
反応性ガス放出機構が配設される反応領域とが設
けられる。 Therefore, as a film formation method that enables a high-quality, uniform thin film without the harmful effects of mercury and without impurities or load particle damage at a sufficiently fast deposition rate for practical use, we have developed a film-forming method using ultraviolet rays irradiated from a plasma. A film is formed by causing a photochemical reaction and depositing a reaction product on a substrate separated from the plasma. The film forming apparatus used in this optical CVD method has a plasma region formed by gas discharge and a substrate on which the film is formed in a single container, and a chemically reactive gas release mechanism is installed. A reaction area is provided.
そして、波長が160nm以下の紫外線を有効に
発光する紫外線放射用ガスと光化学反応性ガスを
適切に供給して成膜するものである。プラズマの
生起方法としては、プラズマ領域に電極を配設
し、直流または低周波交流電圧を印加することに
よりガス放電を起させる方式が用いられる。ま
た、電極には、強力な紫外線を得るために大電力
が投入可能な熱陰極が使用され、そのうち、特に
比較的低温で熱電子放射効率の良いアルカリ土類
金属を高融点金属製コイル表面に塗布したフイラ
メント熱陰極が使用される。このフイラメント熱
陰極は高効率な反面、反応性ガスの水素や酸素等
により著しく劣化する性質を持つことが知られて
いる。 Then, a film is formed by appropriately supplying an ultraviolet radiation gas and a photochemically reactive gas that effectively emit ultraviolet light having a wavelength of 160 nm or less. As a method for generating plasma, a method is used in which an electrode is disposed in a plasma region and a DC or low frequency AC voltage is applied to generate a gas discharge. In addition, a hot cathode is used for the electrode, which can input a large amount of power in order to obtain strong ultraviolet rays. Among them, alkaline earth metals, which have high thermal electron emission efficiency at relatively low temperatures, are used on the surface of the high-melting point metal coil. A coated filament hot cathode is used. Although this filament hot cathode is highly efficient, it is known that it is significantly degraded by reactive gases such as hydrogen and oxygen.
[発明が解決しようとする問題点]
上記のように、電極が配設されるプラズマ領域
と反応性ガスが放出される反応領域とを一つの容
器内に有する成膜装置では、放出された紫外線放
射用ガス、反応性ガスまたは成膜反応時に副成さ
れたガスに含まれる水素、酸素等の反応性ガスが
プラズマ領域にわずかに拡散し、フイラメント熱
陰極の寿命を著しく短くするという問題があつ
た。[Problems to be Solved by the Invention] As described above, in a film forming apparatus having a plasma region in which electrodes are disposed and a reaction region in which reactive gas is emitted in one container, the emitted ultraviolet rays There is a problem in that reactive gases such as hydrogen and oxygen contained in the radiation gas, reactive gas, or gases produced by-product during the film-forming reaction diffuse slightly into the plasma region, significantly shortening the life of the filament hot cathode. Ta.
また、反応性ガスによる劣化がフイラメントに
比較してやや少ないトリエーテツドタングステン
等の熱陰極を使用する場合は、放電を維持するた
めに2000℃以上の高温にしなければならず、装置
の冷却が大がかりになり、実用化が難しく、ま
た、反応性ガスによる劣化が少ない冷陰極を使用
する場合は、放電を維持するためにフイラメント
熱陰極に比べて高電圧が必要であり、電源装置が
大型になり、安定した放電を大電力、低周波で維
持させるのが難しい等の問題があつた。 In addition, when using a hot cathode made of triated tungsten, which is slightly less susceptible to deterioration due to reactive gases than a filament, the temperature must be raised to over 2000°C to maintain discharge, which requires extensive cooling of the device. When using a cold cathode, which is difficult to put into practical use and is less prone to deterioration due to reactive gases, a higher voltage is required to maintain discharge than a filament hot cathode, and the power supply is larger. However, there were problems such as difficulty in maintaining stable discharge at high power and low frequency.
また、電極を使用せずに、高周波やマイクロ波
により放電させる無電極放電をプラズマ生起方法
として使用する場合は、寿命が長い反面、通常成
膜を行う減圧下では、発光効率が電極方式に比べ
て著しく低く、充分な体積速度が得られないとい
う問題があつた。 In addition, when using electrodeless discharge as a plasma generation method using high frequency or microwave without using electrodes, the lifetime is long, but the luminous efficiency is lower than that of the electrode method under the reduced pressure where film formation is normally performed. There was a problem that the volume velocity was extremely low and a sufficient volume velocity could not be obtained.
本発明は、かかる従来の問題点を解決するため
になされたもので、反応性ガスによる電極の劣化
が少なく、長寿命で成膜速度が早く、かつ荷電粒
子による堆積膜損傷も生じない成膜装置を提供す
ることを目的とする。 The present invention has been made in order to solve these conventional problems, and is capable of forming a film with little deterioration of the electrode due to reactive gas, long life, fast film formation speed, and no damage to the deposited film due to charged particles. The purpose is to provide equipment.
[問題点を解決するための手段]
上記の目的を達成するために、この発明の成膜
装置は、プラズマ領域に直流もしくは低周波交流
電圧を印加する電極と、マイクロ波を導入する導
入窓とを設け、前記電極に印加する直流もしくは
低周波交流電圧と、前記導入窓に導入するマイク
ロ波とを同時に加えることによりプラズマを生起
させる構成を有するものである。[Means for Solving the Problems] In order to achieve the above object, the film forming apparatus of the present invention includes an electrode for applying a DC or low frequency AC voltage to a plasma region, and an introduction window for introducing microwaves. The device is configured to generate plasma by simultaneously applying a direct current or low frequency alternating current voltage applied to the electrode and microwave introduced into the introduction window.
[作用]
上記の構成を有することにより、電極間の放電
とマイクロ波の組合せにより、安定したプラズマ
放電が得られ、それによつて成膜の堆積速度も著
しく増加する。[Function] With the above configuration, a stable plasma discharge can be obtained by the combination of the discharge between the electrodes and microwaves, and thereby the deposition rate of film formation can be significantly increased.
[実施例]
以下、図面に示す実施例に基づいて本発明を具
体的に説明する。[Examples] Hereinafter, the present invention will be specifically described based on examples shown in the drawings.
第1図において、容器5内部の上方の空間がプ
ラズマ領域Aであり、下方の空間が反応領域Bで
ある。このプラズマ領域Aには一対の電極1,1
が対向配置され、これに直流または低周波交流電
圧が印加される。この時、電極の負電圧が印加さ
れた片側は冷陰極として動作する。容器5の天井
部には、マイクロ波導入用の石英製の導入窓8が
配置され、導波管9よりマイクロ波MWが導入さ
れる。導入窓8の材質は石英に限られるものでは
なく、マイクロ波を透過する他の材質、さらには
何の材質も必要とせずに単に開口しているだけで
も良い。容器5の上部側面の電極1の背部には、
紫外線放射用ガスG1の導入孔6,6が形成され、
これより稀ガス、水素もしくは重水素、またはこ
れらを含む混合ガスから選ばれた紫外線放射用ガ
スG1が導入される。紫外線放射用ガスG1はマイ
クロ波MWにより、主に導入窓8の近傍で電離さ
れる。この電離されたガスにより電極1,1間の
絶縁破壊が起こり、電極1,1間に電極1,1に
プラズマPが形成され、このプラズマPより放出
される紫外線を含む光が下方の反応領域Bに照射
される。反応領域Bには基板ホルダ3が配置さ
れ、その上に膜形成を行う基板4が載置される。
そして、この少し上方には光化学反応性ガス放出
機構であるリング状のパイプ2が配置され、その
ノズル2aより光化学反応性ガスG2が基板4の
近傍に放出される。従つて、ガスG2が紫外線に
より直接光分解され、反応生成物が基板4上に堆
積して成膜される。基板ホルダ3の下方には排気
口10が設けられ、これから内部のガスが排気さ
れる。また、これらの配置を上下逆にし、基板を
上部に設置することにより、フレーク等が基板に
降りかかるのを防止するのも良い。 In FIG. 1, the upper space inside the container 5 is the plasma region A, and the lower space is the reaction region B. In this plasma region A, a pair of electrodes 1, 1
are arranged facing each other, and a DC or low frequency AC voltage is applied thereto. At this time, one side of the electrode to which a negative voltage is applied operates as a cold cathode. A quartz introduction window 8 for introducing microwaves is arranged on the ceiling of the container 5, and microwaves MW are introduced through a waveguide 9. The material of the introduction window 8 is not limited to quartz, and may be made of other materials that transmit microwaves, or may be simply open without requiring any material. On the back of the electrode 1 on the upper side of the container 5,
Introductory holes 6, 6 for ultraviolet radiation gas G1 are formed,
From this, an ultraviolet radiation gas G 1 selected from a rare gas, hydrogen or deuterium, or a mixed gas containing these gases is introduced. The ultraviolet radiation gas G 1 is ionized mainly in the vicinity of the introduction window 8 by the microwave MW. This ionized gas causes dielectric breakdown between the electrodes 1 and 1, and plasma P is formed between the electrodes 1 and 1, and light including ultraviolet rays emitted from this plasma P is transmitted to the reaction area below. B is irradiated. A substrate holder 3 is arranged in the reaction area B, and a substrate 4 on which a film is to be formed is placed thereon.
A ring-shaped pipe 2, which is a photochemically reactive gas discharge mechanism, is arranged slightly above this, and a photochemically reactive gas G2 is discharged near the substrate 4 from its nozzle 2a. Therefore, the gas G 2 is directly photodecomposed by the ultraviolet rays, and the reaction products are deposited on the substrate 4 to form a film. An exhaust port 10 is provided below the substrate holder 3, through which the gas inside is exhausted. It is also good to prevent flakes and the like from landing on the substrate by placing these upside down and placing the substrate on top.
領域Aと領域Bの間には、プラズマ領域と反応
領域を電気的に区画し、荷電粒子が反応領域に拡
散するのを抑制するために、導電性の隔壁7を配
設するのが良い。隔壁7には基板4の大きさとほ
ぼ等しいか、やや大きな開口部を有し、この開口
部は導電性のシールド網7aで覆われており、両
領域A,Bは隔壁7とシールド網7aで区画され
ている。もつとも、隔壁7を配設せずにシールド
網7aのみで区画してもよいが、図面の如く、隔
壁7の配置によつてシールド網7aの面積を小さ
くすれば、ガスG2が領域Aに拡散するのを減少
させることができる。 A conductive partition wall 7 is preferably disposed between the region A and the region B in order to electrically separate the plasma region and the reaction region and to suppress the diffusion of charged particles into the reaction region. The partition wall 7 has an opening approximately equal to or slightly larger than the substrate 4, and this opening is covered with a conductive shielding net 7a, and both areas A and B are covered by the partitioning wall 7 and the shielding net 7a. It is sectioned. Of course, it may be partitioned by only the shield net 7a without arranging the partition wall 7, but if the area of the shield net 7a is made smaller by arranging the partition wall 7 as shown in the drawing, the gas G 2 can be divided into the area A. Diffusion can be reduced.
これら隔壁7、シールド網7aは、例えばステ
ンレスで製作してもよいが、アモルフアスシリコ
ンを堆積して成膜するときには、これらをシリコ
ン製とするか、表面にシリコン膜を被膜するのが
よい。これは、シールド網7aなどがプラズマに
さらされてスパツタリング現象を起し、スパツタ
されたものが膜中にとり込まれても同じ元素であ
るために膜質を低下させることがないからであ
る。 These partition walls 7 and shield net 7a may be made of stainless steel, for example, but when amorphous silicon is deposited to form a film, it is preferable that they be made of silicon or that their surfaces be coated with a silicon film. This is because even if the shield net 7a and the like are exposed to plasma and a sputtering phenomenon occurs, and the sputtered material is incorporated into the film, the film quality will not deteriorate because the elements are the same.
この実施例においては、電圧印加およびマイク
ロ波によつて生起されたプラズマPが光源として
有効に作用するように、領域Aには紫外線放射用
ガスG1として、稀ガス、水素、重水素およびこ
れらの混合ガスが光化学反応性ガスG2の種類に
応じて選択され、供給される。例えば、アモルフ
アスシリコンを堆積する場合には、ガスG2がシ
ランとすれば、シランは160nm以下の紫外線に
より直接光分解して堆積するから、160nm以下
の紫外線を有効に発光するG1として、アルゴン、
クリプトン、キセノン等が選ばれる。因に、アル
ゴンの発光波長は104.8nm、106.7nm、クリプト
ンは123.6nm、116.5nm、キセノンは147.0nm、
129.6nmである。 In this embodiment, in order that plasma P generated by voltage application and microwaves can effectively act as a light source, region A contains rare gases, hydrogen, deuterium, and other gases as ultraviolet radiation gas G1 . A mixed gas of G2 is selected and supplied depending on the type of photochemically reactive gas G2. For example, when depositing amorphous silicon, if the gas G 2 is silane, silane is deposited by direct photolysis with ultraviolet rays of 160 nm or less, so as G 1 that effectively emits ultraviolet rays of 160 nm or less, Argon,
Krypton, xenon, etc. are selected. Incidentally, the emission wavelengths of argon are 104.8nm and 106.7nm, krypton is 123.6nm and 116.5nm, xenon is 147.0nm,
It is 129.6nm.
さらに、プラズマPはマイクロ波MWにより、
電離したガスにより絶縁破壊されて冷陰極動作の
電極1,1間に生起されるので、マイクロ波MW
を用いない場合に比較して、充分に低い印加電圧
で、かつ安定に大電力放電が維持される。従つ
て、反応性ガスによる電極の劣化が少なく長寿命
で、かつ電源装置が小型となり、さらに、無電極
放電に比べ発光効率が高く有効に成膜される。そ
して、水銀による光増感反応に依らなくても充分
な成膜速度が得られ、水銀による汚染も問題とな
らない。 Furthermore, plasma P is generated by microwave MW,
Microwave MW is generated between electrodes 1 and 1 of cold cathode operation due to dielectric breakdown caused by ionized gas.
Compared to the case without using, high power discharge can be stably maintained at a sufficiently low applied voltage. Therefore, the electrodes are less likely to deteriorate due to reactive gases, resulting in a long life, and the power supply device can be made smaller.Furthermore, the luminous efficiency is higher than in electrodeless discharge, and a film can be formed more effectively. Further, a sufficient film formation rate can be obtained without relying on a photosensitization reaction due to mercury, and contamination due to mercury does not become a problem.
また、プラズマPの荷電粒子が領域Bに拡散し
ようとしても、シールド網7aでその殆どが捕捉
されて基板4に到達しないので、堆積膜は荷電粒
子による損傷を受けず、かつ不純物の混入も少な
くて性能の優れた堆積膜を得ることができる。 Furthermore, even if the charged particles of the plasma P try to diffuse into the region B, most of them are captured by the shield network 7a and do not reach the substrate 4, so the deposited film is not damaged by the charged particles and there is less contamination of impurities. It is possible to obtain a deposited film with excellent performance.
次に、第1図に示す成膜装置における成膜例を
示すと、容器内圧力が0.7mmHg、基板温度が250
℃の条件でアモルフアスシリコンの薄膜を堆積さ
せる場合、紫外線放射用ガスG1がアルゴンで流
量100sccm、光化学反応性ガスG2がシランで流量
20sccm流し、マイクロ波導入窓13より周波数
2.45GHz、電力400Wのマイクロ波を導入し、こ
れと同時に電極1,1間に周波数50Hz、電圧
230Vを印加すると、電極1,1間で放電が開始
され、この時の電極1,1間の放電電圧が180V、
電流が4Aで安定してプラズマPが生起し、1.1〜
1.31Å/秒の高速な堆積速度で成膜できた。得ら
れた薄膜は荷電粒子損傷のない良好なものであ
り、光導電率はσp=10-4S/cm、暗導電率はσd=
10-9S/cmであつて高品質の薄膜となつた。また、
電極の寿命は大巾に寿命が延びた。 Next, an example of film formation using the film forming apparatus shown in Fig. 1 is shown.
When depositing a thin film of amorphous silicon under conditions of ℃, the ultraviolet radiation gas G 1 is argon at a flow rate of 100 sccm, and the photochemically reactive gas G 2 is silane at a flow rate of 100 sccm.
20 sccm flow, frequency from microwave introduction window 13
A microwave with a frequency of 2.45 GHz and a power of 400 W was introduced, and at the same time, a frequency of 50 Hz and a voltage was applied between electrodes 1 and 1.
When 230V is applied, discharge starts between electrodes 1 and 1, and the discharge voltage between electrodes 1 and 1 at this time is 180V,
The current is stable at 4A, plasma P is generated, and 1.1~
The film could be formed at a high deposition rate of 1.31 Å/sec. The obtained thin film was in good condition with no charged particle damage, the photoconductivity was σ p =10 -4 S/cm, and the dark conductivity was σ d =
10 -9 S/cm, resulting in a high quality thin film. Also,
The lifespan of the electrodes has been significantly extended.
第2図はマイクロ波電力に対する堆積速度を示
したもので、400W程度の小電力で充分な堆積速
度が得られることを示しており、これは同じ電力
のマイクロ波だけによる放電発光を用いた場合の
堆積速度の20倍であり、電極1,1間の放電とマ
イクロ波を組合せることにより、飛躍的に堆積速
度が増加することを示している。 Figure 2 shows the deposition rate versus microwave power, and shows that a sufficient deposition rate can be obtained with a small power of about 400W, which is the same as when using discharge light emission using only microwaves of the same power. This shows that the deposition rate can be dramatically increased by combining the electric discharge between the electrodes 1 and microwaves.
一方、マイクロ波を用いずに冷陰極動作の電極
だけの放電で成膜しようとした場合は、放電を開
始させるのに、600V以上の高電圧が必要であり、
また、生起した放電は不安定ですぐに停止してし
まい、成膜することができなかつた。 On the other hand, if you try to form a film by discharging only the cold cathode electrode without using microwaves, a high voltage of 600V or more is required to start the discharge.
Further, the discharge that occurred was unstable and stopped immediately, making it impossible to form a film.
また、最初の電極放電開始時のみにマイクロ波
を導入し、放電開始後にマイクロ波を停止し、電
極のみの動作とした場合は、マイクロ波を停止す
ると、ただちにプラズマ放電が停止してしまい、
成膜することができなかつた。 In addition, if microwaves are introduced only when the first electrode discharge starts, and then the microwaves are stopped after the discharge starts and only the electrodes are operated, the plasma discharge will stop immediately when the microwaves are stopped.
It was not possible to form a film.
尚、前記実施例では、反応性ガスがプラズマか
ら放射される紫外線によつて反応が開始される光
CVD法について述べたが、これに限られるもの
ではなく、反応性ガスがプラズマ領域から拡散さ
れる励起された中性粒子、例えば電子励起された
アルゴンのAr(3P2)等によつて反応が開始され
る励起種CVD法に適用しても、同様の効果が得
られ、さらには、光と励起種の両方を組合せた
CVD法に適用しても同様の効果が得られる。 Incidentally, in the above embodiment, the reaction of the reactive gas is initiated by the ultraviolet rays emitted from the plasma.
Although we have mentioned CVD methods, but are not limited to them, reactive gases are diffused from the plasma region by excited neutral particles, such as electronically excited argon Ar ( 3P2 ), etc. A similar effect can be obtained when applied to the excited species CVD method in which the reaction is initiated, and even more
A similar effect can be obtained when applied to the CVD method.
[発明の効果]
以上説明した様に、本発明にかかる成膜装置
は、プラズマ領域に直流または低周波交流電圧を
印加する電極と、マイクロ波を導入する導入窓を
有し、直流または低周波交流電圧とマイクロ波を
同時に加えることによりプラズマを生起させるの
で、電極に反応性ガスによる劣化の少ない冷陰極
動作の電極を使用することができ、安定なプラズ
マを生起させることができると共に、長寿命で高
速堆積をすることが可能となり、堆積膜に対して
不純物や荷電粒子損傷がないので、高品質で均一
な薄膜を堆積させることができる等、多くの利点
を有する。[Effects of the Invention] As explained above, the film forming apparatus according to the present invention has an electrode for applying a DC or low frequency AC voltage to a plasma region and an introduction window for introducing microwaves, and has an electrode for applying a DC or low frequency AC voltage to a plasma region. Plasma is generated by applying AC voltage and microwave simultaneously, so cold cathode operation electrodes that are less susceptible to deterioration due to reactive gases can be used, making it possible to generate stable plasma and have a long service life. It has many advantages, such as high-speed deposition, no impurity or charged particle damage to the deposited film, and the ability to deposit high-quality, uniform thin films.
第1図は本発明の一実施例を示す成膜装置の断
面図、第2図は第1図の装置で導入するマイクロ
波の電力を変化させたときのマイクロ波電力の変
化に対する堆積速度を示す図である。
図中、1…電極、2…パイプ、2a…ノズル、
3…基板ホルダ、4…基板、5…容器、6…導入
孔、7…隔壁、7a…シールド網、8…導入窓、
9…導波管、10…排気口、P…プラズマ、G1
…紫外線放射用ガス、G2…光化学反応性ガス。
Fig. 1 is a cross-sectional view of a film forming apparatus showing an embodiment of the present invention, and Fig. 2 shows the deposition rate with respect to the change in microwave power when the power of the microwave introduced in the apparatus of Fig. 1 is changed. FIG. In the figure, 1... electrode, 2... pipe, 2a... nozzle,
3... Substrate holder, 4... Substrate, 5... Container, 6... Introduction hole, 7... Partition wall, 7a... Shield net, 8... Introduction window,
9... Waveguide, 10... Exhaust port, P... Plasma, G 1
...gas for ultraviolet radiation, G 2 ...photochemically reactive gas.
Claims (1)
ガス放電によつて形成されるプラズマ領域と、反
応性ガス放出機構が配設された反応領域とを有す
る成膜装置において、前記プラズマ領域に直流も
しくは低周波交流電圧を印加する電極と、マイク
ロ波を導入する導入窓とを設け、前記電極に印加
する直流もしくは低周波交流電圧と、前記導入窓
に導入するマイクロ波とを同時に加えることによ
りプラズマを生起させる手段を具備したことを特
徴とする成膜装置。 2 反応性ガスは、プラズマ領域から放射される
紫外線によつて反応が開始されることを特徴とす
る特許請求の範囲第1項記載の成膜装置。 3 反応性ガスは、プラズマ領域から拡散される
励起された中性粒子によつて反応が開始されるこ
とを特徴とする特許請求の範囲第1項記載の成膜
装置。[Scope of Claims] 1. Film formation having a plasma region formed by gas discharge and a reaction region provided with a reactive gas release mechanism in one container provided with a substrate for film formation. In the apparatus, an electrode for applying a DC or low frequency AC voltage to the plasma region and an introduction window for introducing microwaves are provided, and the DC or low frequency AC voltage applied to the electrode and the micro wave introduced to the introduction window are provided. 1. A film forming apparatus characterized by comprising means for generating plasma by simultaneously applying waves. 2. The film forming apparatus according to claim 1, wherein the reaction of the reactive gas is initiated by ultraviolet rays emitted from the plasma region. 3. The film forming apparatus according to claim 1, wherein the reaction of the reactive gas is initiated by excited neutral particles diffused from the plasma region.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62062666A JPS63229711A (en) | 1987-03-19 | 1987-03-19 | Film formation device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62062666A JPS63229711A (en) | 1987-03-19 | 1987-03-19 | Film formation device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63229711A JPS63229711A (en) | 1988-09-26 |
| JPH0533812B2 true JPH0533812B2 (en) | 1993-05-20 |
Family
ID=13206844
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62062666A Granted JPS63229711A (en) | 1987-03-19 | 1987-03-19 | Film formation device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS63229711A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0477229U (en) * | 1990-11-20 | 1992-07-06 | ||
| JP5836144B2 (en) * | 2012-01-31 | 2015-12-24 | 東京エレクトロン株式会社 | Microwave radiation mechanism and surface wave plasma processing equipment |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4042850A (en) * | 1976-03-17 | 1977-08-16 | Fusion Systems Corporation | Microwave generated radiation apparatus |
| JPS58159842A (en) * | 1982-03-17 | 1983-09-22 | Ricoh Co Ltd | Manufacture of photoreceptor |
| JPS61241930A (en) * | 1985-04-18 | 1986-10-28 | Matsushita Electric Ind Co Ltd | Plasma chemical vapor deposition device |
| US4582773A (en) * | 1985-05-02 | 1986-04-15 | Energy Conversion Devices, Inc. | Electrophotographic photoreceptor and method for the fabrication thereof |
-
1987
- 1987-03-19 JP JP62062666A patent/JPS63229711A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63229711A (en) | 1988-09-26 |
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