JPS63214345A - Plasma processing apparatus - Google Patents

Plasma processing apparatus

Info

Publication number
JPS63214345A
JPS63214345A JP4636587A JP4636587A JPS63214345A JP S63214345 A JPS63214345 A JP S63214345A JP 4636587 A JP4636587 A JP 4636587A JP 4636587 A JP4636587 A JP 4636587A JP S63214345 A JPS63214345 A JP S63214345A
Authority
JP
Japan
Prior art keywords
chamber
plasma generation
plasma
sample
generation 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
JP4636587A
Other languages
Japanese (ja)
Inventor
Kyoichi Komachi
小町 恭一
Sumio Kobayashi
純夫 小林
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.)
Nippon Steel Corp
Original Assignee
Sumitomo Metal Industries 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 Sumitomo Metal Industries Ltd filed Critical Sumitomo Metal Industries Ltd
Priority to JP4636587A priority Critical patent/JPS63214345A/en
Publication of JPS63214345A publication Critical patent/JPS63214345A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/32Gas-filled discharge tubes
    • H01J37/32009Arrangements for generation of plasma specially adapted for examination or treatment of objects, e.g. plasma sources
    • H01J37/32192Microwave generated discharge

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Physical Or Chemical Processes And Apparatus (AREA)
  • Crystals, And After-Treatments Of Crystals (AREA)
  • Chemical Vapour Deposition (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は主にCVD(Che+5ical Vapor
 Deposition)装置等として用いられるプラ
ズマプロセス装置に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention mainly applies to CVD (Che+5ical vapor
The present invention relates to a plasma processing apparatus used as a deposition apparatus, etc.

〔従来技術〕[Prior art]

一般に低温プラズマを発生させるための励起手段として
ラジオ波(RF波)を用いる場合とマイクロ波を用いる
場合があるが、マイクロ波はラジオ波を用いる場合と比
較してより低温で、且つ高密度のプラズマを得られるこ
と、電極による汚染がないこと、装置並びにその操作が
簡単であること等の利点がある。
In general, radio waves (RF waves) or microwaves are used as an excitation means for generating low-temperature plasma, but microwaves have lower temperature and higher density than radio waves. It has advantages such as being able to obtain plasma, being free from electrode contamination, and being easy to use and operate the device.

マイクロ波を利用するプラズマプロセス装置としては従
来電子サイクロトロン共鳴(ECR)方式が広く知られ
ているが(特開昭55−141729号)、この方式は
磁場を利用するため指向性が良いこと、また高真空下で
プラズマを生成するため膜質が良い利点を有する反面、
処理面積が小さいという難点があった。この電子サイク
ロトロン共鳴方式よりも広い処理面積が得られる方式と
してマイクロ波をアンテナにてプラズマ生成室に導入す
る方式(特開昭56−41382号、 57−9868
号)もあるが、この方式はアンテナとの整合が難しく、
プラズマ分布が不均一になり易いという難点があった。
Conventionally, the electron cyclotron resonance (ECR) method is widely known as a plasma processing device that uses microwaves (Japanese Patent Application Laid-open No. 141729/1983), but this method uses a magnetic field, so it has good directivity, and Although it has the advantage of good film quality because plasma is generated under high vacuum,
The problem was that the processing area was small. A method that can obtain a larger processing area than this electron cyclotron resonance method is a method in which microwaves are introduced into the plasma generation chamber using an antenna (Japanese Patent Application Laid-Open No. 56-41382, 57-9868).
), but this method is difficult to match with the antenna,
There was a problem that the plasma distribution tended to become non-uniform.

このため近時にあっては処理面積が極めて大きく、しか
も整合等の操作も容易なはしご状周期構造を利用する方
式(The Large Volume Microw
avePlasma Generator J、 Mi
crowave Power 7 (4)1972) 
、或いは誘電体被覆線路を利用する方式等が試みられて
おり、誘電体被覆線路を利用する方式については本発明
者等は既に提案を行っである(特願昭60−14303
6号、 60−240070号)。
For this reason, in recent years, a method using a ladder-like periodic structure (The Large Volume Micro
avePlasma Generator J, Mi
Crowave Power 7 (4) 1972)
Alternatively, methods using dielectric covered lines have been attempted, and the present inventors have already proposed a method using dielectric covered lines (Japanese Patent Application No. 14303/1986).
No. 6, No. 60-240070).

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

ところで上述した如き方式のプラズマプロセス装置は処
理面積を広く設定出来る反面、プラズマの指向性が十分
でなく、処理の均一性に問題があり、また試料をプラズ
マ生成室内に配するため成膜時におけるイオン衝撃が大
きく膜質が悪く、更に反応性ガスをプラズマ生成室内に
供給したときプラズマ生成室内壁面への膜付着量が多く
なり、プラズマの発生が不安定になる等の問題があった
By the way, although the plasma processing apparatus of the above-mentioned type can set a wide processing area, the directivity of the plasma is not sufficient and there is a problem with the uniformity of processing.Also, since the sample is placed inside the plasma generation chamber, there are problems during film formation. There were problems such as large ion bombardment, poor film quality, and furthermore, when a reactive gas was supplied into the plasma generation chamber, a large amount of film was deposited on the wall surface of the plasma generation chamber, making plasma generation unstable.

本発明はかかる事情に鑑みなされたものであって、その
目的とするところはマイクロ波を用いて大面積にプラズ
マを発生させると共に、指向性を高めて試料面に対する
均一な処理を可能ならしめ、またプラズマ生成室壁面へ
の膜付着を解消し、プラズマ発生の不安定を防止すると
共に、反応ガスの有効利用を図れるようにしたプラズマ
プロセス装置を提供するにある。
The present invention has been developed in view of the above circumstances, and its purpose is to generate plasma over a large area using microwaves, increase directivity, and enable uniform treatment of the sample surface. Another object of the present invention is to provide a plasma processing apparatus that eliminates film adhesion to the wall surface of a plasma generation chamber, prevents instability of plasma generation, and enables effective use of reaction gas.

〔問題点を解決するための手段〕[Means for solving problems]

本発明装置にあっては、少なくとも一部をマイクロ波の
透過可能な耐熱壁で形成されたプラズマ生成室と、試料
を配設する試料処理室と、試料処理室に沿って前記プラ
ズマ生成室内にマイクロ波の定在波が形成されるようマ
イクロ波を導入する手段と、前記プラズマ生成室を区画
して形成され、定在波の節を含む電界強度の小さい室及
び定在波の腹を含む電界強度の大きい室と、マイクロ波
を遮断する材質で形成されており、前記プラズマ生成室
と試料処理室とを隔てるべく配設され、前記各電界強度
の小さい室及び電界強度の大きい室夫々と試料処理室と
を結ぶ連通口を開設した仕切壁とを具備する。
The apparatus of the present invention includes a plasma generation chamber at least partially formed of a heat-resistant wall through which microwaves can pass, a sample processing chamber in which a sample is placed, and a plasma generation chamber along the sample processing chamber. a means for introducing microwaves so that a standing microwave wave is formed; and a chamber formed by dividing the plasma generation chamber and having a low electric field strength including a node of the standing wave and an antinode of the standing wave. A chamber with a high electric field strength and a material that blocks microwaves are arranged to separate the plasma generation chamber and the sample processing chamber, and each chamber with a low electric field strength and a chamber with a high electric field strength are arranged to separate the plasma generation chamber and the sample processing chamber. It is equipped with a partition wall with a communication port connecting it to the sample processing room.

〔作用〕[Effect]

本発明にあってはこれによって試料に対し均一に指向せ
しめ得、しかもプラズマ生成室内面への膜付着を解消し
て、プラズマ発生を安定させると共に、反応ガス等の有
効利用も図れる。
According to the present invention, this makes it possible to uniformly direct the plasma toward the sample, eliminate film adhesion to the inside of the plasma generation chamber, stabilize plasma generation, and effectively utilize reactant gas and the like.

〔実施例〕〔Example〕

以下本発明をその実施例を示す図面に基づき具体的に説
明する。第1図は本発明に係るプラズマプロセス装置(
以下本発明装置という)の模式的断面図であり、図中1
は反応器、2は誘電体被覆線路を示している。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be specifically described below based on drawings showing embodiments thereof. FIG. 1 shows a plasma process apparatus (
1 is a schematic cross-sectional view of the device (hereinafter referred to as the device of the present invention).
2 shows a reactor, and 2 shows a dielectric covered line.

反応器1にはガス導入系3、排気系4が連結され、また
誘電体被覆線路2には導波管5を介してマイクロ波発振
器6が連結されており、誘電体被覆線路2はこれを略水
平に配置し、一方反応器1は誘電体被覆線路2下にあっ
てその上面が導波管5側に向くよう若干傾斜させて配設
されている。
A gas introduction system 3 and an exhaust system 4 are connected to the reactor 1, and a microwave oscillator 6 is connected to the dielectric covered line 2 via a waveguide 5; The reactor 1 is arranged substantially horizontally, while the reactor 1 is located below the dielectric covered line 2 and is arranged slightly inclined so that its upper surface faces the waveguide 5 side.

第2図(イ)は反応器lの拡大断面図、第2図(ロ)は
反応器内のプラズマ生成室に形成されるマイクロ波の定
在波の波形図であり、反応器1は中空直方体形であって
上部壁を除く全体が金属製であり、特に周囲壁は二重構
造であって内部に冷却水用の通流室11を備えている0
反応器1の上部壁はマイクロ波の透過が可能な誘電損失
の小さな耐熱性板12、例えば石英ガラス又はパイレッ
クスガラス等にて気密状態に封止され、この誘電損失の
小さな耐熱性板12に対向させて前記した誘電体被覆線
路2が対向配置されている。
Figure 2 (a) is an enlarged sectional view of reactor 1, and Figure 2 (b) is a waveform diagram of standing microwave waves formed in the plasma generation chamber inside the reactor. It has a rectangular parallelepiped shape and is entirely made of metal except for the upper wall, and the surrounding wall in particular has a double structure and is equipped with a circulation chamber 11 for cooling water inside.
The upper wall of the reactor 1 is hermetically sealed with a heat-resistant plate 12 with low dielectric loss that allows microwave transmission, such as quartz glass or Pyrex glass, and is opposed to this heat-resistant plate 12 with low dielectric loss. The dielectric covered lines 2 described above are arranged facing each other.

反応器1の内部は上端側寄りの位置で耐熱性板12と平
行に配した仕切壁13にて上、下に区分され、仕切壁1
3の上部はプラズマ生成室14とし、また仕切壁13の
下部は試料処理室15としてあり、前記プラズマ生成室
14内にはその上部の耐熱性板12を透過してマイクロ
波が導入され、ここに第2図(ロ)に示す如き定在波が
形成されようにしである。
The inside of the reactor 1 is divided into upper and lower parts by a partition wall 13 arranged parallel to the heat-resistant plate 12 near the upper end.
The upper part of 3 is a plasma generation chamber 14, and the lower part of the partition wall 13 is a sample processing chamber 15. Microwaves are introduced into the plasma generation chamber 14 by passing through the heat-resistant plate 12 at the upper part. A standing wave as shown in FIG. 2(b) is likely to be formed.

プラズマ生成室14内は隔壁14aを仕切壁13と、耐
熱性板12との間に渡して定在波の節を含む電界強度の
小さい室A+ と定在波の腹を含む電界強度の大きい室
A0とに区分されており、定在波の腹を含む電界強度の
大きい室A0はその一端部においてガス供給系3を構成
するプラズマ用原料ガスの供給管3aが、また定在波の
節を含む電界強度の小さい室A、はその一端部において
同じくガス供給系3を構成する反応性ガスの供給管3b
が夫々連結せしめられている。一方試料処理室15は排
気系4を構成する排気管4aと連結され、内部には試料
16が図示しない支持台上に前に仕切壁13と所要の間
隔βを隔てて略これと平行に配設されている。
Inside the plasma generation chamber 14, a partition wall 14a is passed between the partition wall 13 and the heat-resistant plate 12 to create a chamber A+ with a low electric field strength that includes nodes of standing waves and a chamber with a high electric field strength that includes antinodes of standing waves. The chamber A0, which has a large electric field strength including the antinode of the standing wave, has a supply pipe 3a for plasma source gas constituting the gas supply system 3 at one end, and a chamber A0 which has a node of the standing wave. The chamber A containing a small electric field strength has a reactive gas supply pipe 3b, which also constitutes the gas supply system 3, at one end thereof.
are connected to each other. On the other hand, the sample processing chamber 15 is connected to an exhaust pipe 4a constituting the exhaust system 4, and inside the sample 16 is arranged on a support (not shown) in front of the partition wall 13 at a required distance β and substantially parallel to the partition wall 13. It is set up.

仕切壁13はマイクロ波を遮蔽し得る物質、主としてス
テンレス鋼等の金属にて形成されており、これには室A
o 、A+夫々と対向する位置に試料処理室15と通ず
るスリット状の連通口13a、 13bが開口せしめら
れており、室A0に供給されたガスはプラズマ分解され
、発生したプラズマ、ラジカル等は連通口13aを通じ
て、また室Alに供給された反応性ガスは若干励起され
た状態で連通口13bを通じて夫々室A、、A、と試料
処理室15との間に形成された圧力差に依って試料処理
室15内に導出され、試料16表面に指向せしめ得るよ
うにしである。
The partition wall 13 is made of a material capable of shielding microwaves, mainly metal such as stainless steel.
Slit-shaped communication ports 13a and 13b communicating with the sample processing chamber 15 are opened at positions facing O and A+, respectively, and the gas supplied to the chamber A0 is plasma decomposed, and the generated plasma, radicals, etc. are communicated. The reactive gas supplied to the chamber Al through the port 13a is slightly excited and then passes through the communication port 13b to the sample processing chamber 15 due to the pressure difference formed between the chambers A, A and the sample processing chamber 15. It is designed so that it can be guided into the processing chamber 15 and directed toward the surface of the sample 16.

連通口13a、 13bの形状はスリット状とした場合
につき説明したが何らこれに限るものではな(、例えば
円形、角形の細孔を多数開設しても良いことは勿論であ
る。
Although the shape of the communication ports 13a and 13b has been described as a slit shape, the shape is not limited to this in any way (for example, it is of course possible to have a large number of circular or square pores).

試料16と仕切壁13との間の寸法lについては特にこ
れに限るものではないが、例えばガスの平均自由行程を
λとしてβ≦λとなるよう設定すればプラズマは粒子間
の衝突なく試料16に到達し得ることとなって、上向性
に優れたプラズマビームを得ることが出来る。
The dimension l between the sample 16 and the partition wall 13 is not particularly limited to this, but for example, if the mean free path of the gas is λ and it is set so that β≦λ, the plasma will move between the sample 16 and the sample 16 without collision between particles. As a result, a plasma beam with excellent upward movement can be obtained.

なお、!を小さくすればビームの広がりが小さく、ビー
ム中のイオン量が多くなり、逆にlを大きくすればビー
ムの広がりが大きく、ビームの殆どはラジカルビームと
なるから試料16の大きさ、ビームの性質等を勘案して
寸法iを定めればよい。
In addition,! If l is made small, the beam spread will be small and the amount of ions in the beam will be large. Conversely, if l is made large, the beam spread will be large and most of the beam will be a radical beam, so the size of the sample 16 and the properties of the beam will be The dimension i may be determined by taking these factors into consideration.

なお、上記の実施例ではプラズマ生成室14と試料処理
室15との圧力差をガス供給系3、排気系4の制御によ
って行う場合につき説明したが、何らこれに限るもので
はな(、仕切壁13の連通口13a。
In the above embodiment, the case where the pressure difference between the plasma generation chamber 14 and the sample processing chamber 15 is controlled by controlling the gas supply system 3 and the exhaust system 4 has been described, but this is not limited to this. 13 communication port 13a.

13bの大きさ、個数を変えることによって圧力差を変
更すこととしてもよい。
The pressure difference may be changed by changing the size and number of the 13b.

また、プラズマ生成室と試料処理室を差動排気すること
によって圧力差を変えることもできる。
Furthermore, the pressure difference can be changed by differentially pumping the plasma generation chamber and sample processing chamber.

一方、誘電体被覆線路2は反応器lの上面を覆い得る広
さのAI製の板2aの下面であって、耐熱製板12の上
面と対向する領域に誘電体層2bを固定して構成され、
その一端側周縁は導波管5に連結され、また他端部には
反射板2cを固定して構成しである。
On the other hand, the dielectric covered line 2 is constructed by fixing a dielectric layer 2b to the lower surface of an AI plate 2a that is large enough to cover the upper surface of the reactor l and facing the upper surface of the heat-resistant plate 12. is,
One end of the periphery is connected to the waveguide 5, and the other end has a reflecting plate 2c fixed thereto.

誘電体層2bの材料としてはテフロン、ポリスチレン、
ポリエチレン等の誘電損失の小さい物質が採用されてい
る。
Materials for the dielectric layer 2b include Teflon, polystyrene,
A material with low dielectric loss, such as polyethylene, is used.

誘電体層2bは表面波導波路として電磁界を集中させ、
耐熱性板12を通じてプラズマ生成室14の室A6.A
Iに導入する。
The dielectric layer 2b concentrates the electromagnetic field as a surface wave waveguide,
Chamber A6 of the plasma generation chamber 14 through the heat-resistant plate 12. A
Introduced into I.

而して上述した如き本発明装置にあっては反応器1内の
プラズマ生成室14の室A0.A、 、試料処理室15
内を所定の真空度に設定した後、図示しないヒータにて
試料16を加熱しつつ、プラズマ生成室14内の室A、
には反応性ガスを、また室A0にはAr等のプラズマ用
原料ガスを夫々ガス供給系3の供給管3a、3bを通じ
てガスを供給すると共に、誘電体被覆線路2を通じてプ
ラズマ生成室14内にマイクロ波を供給する。プラズマ
生成室14の室へ〇に供給されるArガスは強い電界に
よって励起され、プラズマ分解されて、−大室AIに供
給された反応性ガスは軽く励起されるがプラズマ化され
ることなく、各室A・、AI と試料処理室15との圧
力差に従い仕切壁13の連通口13a、 13bを通じ
て試料処理室15内に引出され、試料16の表面に到達
し、気相反応して成膜がなされることとなる。
In the apparatus of the present invention as described above, chamber A0. of the plasma generation chamber 14 in the reactor 1. A. , Sample processing chamber 15
After setting the inside to a predetermined degree of vacuum, the chamber A in the plasma generation chamber 14 is heated while the sample 16 is heated with a heater (not shown).
A reactive gas is supplied to the chamber A0, and a raw material gas for plasma such as Ar is supplied to the chamber A0 through the supply pipes 3a and 3b of the gas supply system 3, respectively. Supply microwave. The Ar gas supplied to the chamber ○ of the plasma generation chamber 14 is excited by a strong electric field and is plasma decomposed, and the reactive gas supplied to the large chamber AI is lightly excited but is not turned into plasma. According to the pressure difference between each chamber A, AI and the sample processing chamber 15, the sample is drawn out into the sample processing chamber 15 through the communication ports 13a and 13b of the partition wall 13, reaches the surface of the sample 16, and undergoes a gas phase reaction to form a film. will be done.

従って室A、内では反応性ガスが存在しないため、ここ
で膜が発生することがな(プラズマの発生は安定維持さ
れることとなる。
Therefore, since there is no reactive gas in chamber A, no film is generated here (the generation of plasma is maintained stably).

〔試験例〕[Test example]

反応器1の寸法諸元、並びに試験条件は次のとおりであ
る。
The dimensions and test conditions of reactor 1 are as follows.

反応器1の仕切壁13としては厚さ1酊の5tlS30
4綱板を用い、またプラズマ生成室14はマイクロ波の
進行方向に318龍、幅200龍とし、マイクロ波の進
行方向に定在波の172波長に相当する略53龍毎に区
分して室As 、A+を形成し、各室A6゜A、と対向
する部分の仕切壁13には試料処理室15と連通する連
通口13a、 13bとして夫々幅0.1mmのスリッ
ト状の連通口を開口した。
The partition wall 13 of the reactor 1 is 5tlS30 with a thickness of 1.
A four-wire plate is used, and the plasma generation chamber 14 has 318 lengths in the direction of microwave propagation and 200 lengths in width, and is divided into approximately 53 lengths in the direction of microwave propagation, which corresponds to 172 wavelengths of the standing wave. Slit-shaped communication ports with a width of 0.1 mm were opened as communication ports 13a and 13b communicating with the sample processing chamber 15, respectively, in the partition wall 13 at the portion facing each chamber A6°A. .

一方誘電体被覆線路2は幅600HのAl製のフレーム
下面に誘電体物質としてテフロンを貼り付けて構成しで
ある。テフロンのマイクロ波進行方向における長さは4
84 m、輻200B、厚さ20mmのものを使用した
。またテフロン下面と耐熱性板12との間の距離は80
m+とじた。
On the other hand, the dielectric covered line 2 is constructed by pasting Teflon as a dielectric material on the lower surface of an Al frame having a width of 600H. The length of Teflon in the microwave propagation direction is 4
84 m, diameter 200B, and thickness 20 mm were used. Also, the distance between the Teflon lower surface and the heat-resistant plate 12 is 80 mm.
m+ closed.

ガス供給系3からは室A0にはN2ガスを、また室A、
にはSiH,を夫々供給し、試料処理室15内に配した
6インチSiウェーハ上に対する成膜を行った結果、略
均−なSiN膜の堆積が認められた。
From gas supply system 3, N2 gas is supplied to chamber A0, and chamber A,
As a result, a substantially uniform SiN film was deposited on a 6-inch Si wafer placed in the sample processing chamber 15.

なお、上述の実施例はCVD装置に適用した場合につき
説明したが、これにかぎらず例えばエピタキシャル成長
装置、アモルファスシリコンの製造装置、その他有機七
ツマ−を用いた有機重合膜の形成等にも適用し得ること
は言うまでもない。
Although the above-mentioned embodiments have been described with reference to the case where they are applied to a CVD apparatus, the present invention is not limited to this, but can also be applied to, for example, an epitaxial growth apparatus, an amorphous silicon manufacturing apparatus, and the formation of an organic polymer film using an organic diammonium. Needless to say, you can get it.

第3図は本発明の他の実施例を示す模式図であり、耐熱
性板12の上方に四角錐形にホーン19を配設し、その
上端に導波管5を縦向きに接続して構成してあり、マイ
クロ波は耐熱性板12に垂直に入射せしめられるように
なっている。
FIG. 3 is a schematic diagram showing another embodiment of the present invention, in which a horn 19 is arranged in the shape of a square pyramid above the heat-resistant plate 12, and a waveguide 5 is vertically connected to the upper end of the horn 19. The structure is such that the microwave is made to enter the heat-resistant plate 12 perpendicularly.

〔効果〕〔effect〕

以上の如く本発明装置にあってはプラズマ生成室内をマ
イクロ波の定在波の節を含む電界強度の小さい室と腹を
含む電界強度の大きい室とに区分し、反応性ガス等は電
界強度の小さい室を通じて試料処理室に供給するように
したから、プラズマ生成室の内壁に膜が付着されること
がなく、安定したプラズマ発生を維持し得、またイオン
衝撃の少ない良質の成膜を行うことが可能となり、また
プラズマの発生は発生しやすい低真空で、処理は汚染の
少ないより高真空で行うことができるなど本発明は優れ
た効果を奏するものである。
As described above, in the apparatus of the present invention, the plasma generation chamber is divided into a chamber with a low electric field strength including nodes of microwave standing waves and a chamber with a high electric field strength including an antinode, and reactive gases etc. are Since the plasma is supplied to the sample processing chamber through a small chamber, the film does not adhere to the inner wall of the plasma generation chamber, allowing stable plasma generation to be maintained and high-quality film formation with less ion bombardment. The present invention has excellent effects such as being able to perform processing in a low vacuum where plasma is easily generated and in a high vacuum where there is less contamination.

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

第1図は本発明装置の模式図、第2図は本発明装置にお
ける反応容器とそのプラズマ生成室に形成するマイクロ
波の定在波の波形との位置関係を示す説明図、第3図は
本発明の他の実施例を示す模式図である。 1・・・反応器 2・・・誘電体被覆線路 3・・・ガ
ス供給系 4・・・排気系 5・・・導波管 6・・・
マイクロ波発振器 12・・・耐熱性板 13・・・仕
切壁13a、 13b・・・連通口 14・・・プラズ
マ生成室 15・・・試料処理室 16・・・試料 A
o、A+・・・家持 許 出願人  住友金属工業株式
会社代理人 弁理士  河  野  登  失策 3 
Figure 1 is a schematic diagram of the apparatus of the present invention, Figure 2 is an explanatory diagram showing the positional relationship between the reaction vessel in the apparatus of the present invention and the waveform of the microwave standing wave formed in its plasma generation chamber, and Figure 3 is It is a schematic diagram which shows another Example of this invention. 1...Reactor 2...Dielectric coated line 3...Gas supply system 4...Exhaust system 5...Waveguide 6...
Microwave oscillator 12... Heat-resistant plate 13... Partition walls 13a, 13b... Communication port 14... Plasma generation chamber 15... Sample processing chamber 16... Sample A
o, A+... Home ownership Applicant Sumitomo Metal Industries Co., Ltd. Agent Patent attorney Noboru Kono Mistake 3
figure

Claims (1)

【特許請求の範囲】[Claims] 1、少なくとも一部をマイクロ波の透過可能な耐熱壁で
形成されたプラズマ生成室と、試料を配設する試料処理
室と、試料処理室に沿って前記プラズマ生成室内にマイ
クロ波の定在波が形成されるようマイクロ波を導入する
手段と、前記プラズマ生成室を区画して形成され、定在
波の節を含む電界強度の小さい室及び定在波の腹を含む
電界強度の大きい室と、マイクロ波を遮断する材質で形
成されており、前記プラズマ生成室と試料処理室とを隔
てるべく配設され、前記各電界強度の小さい室及び電界
強度の大きい室夫々と試料処理室とを結ぶ連通口を開設
した仕切壁とを具備することを特徴とするプラズマプロ
セス装置。
1. A plasma generation chamber at least partially formed of a heat-resistant wall through which microwaves can pass, a sample processing chamber in which a sample is placed, and a microwave standing wave in the plasma generation chamber along the sample processing chamber. a means for introducing microwaves so that the plasma generation chamber is formed, and a chamber with a low electric field strength including nodes of standing waves and a chamber with high electric field strength including an antinode of the standing waves, which are formed by dividing the plasma generation chamber. , is formed of a material that blocks microwaves, is arranged to separate the plasma generation chamber from the sample processing chamber, and connects each of the chambers with low electric field strength and the chamber with high electric field strength to the sample treatment chamber. A plasma processing device characterized by comprising a partition wall having a communication port.
JP4636587A 1987-02-27 1987-02-27 Plasma processing apparatus Pending JPS63214345A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4636587A JPS63214345A (en) 1987-02-27 1987-02-27 Plasma processing apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4636587A JPS63214345A (en) 1987-02-27 1987-02-27 Plasma processing apparatus

Publications (1)

Publication Number Publication Date
JPS63214345A true JPS63214345A (en) 1988-09-07

Family

ID=12745127

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4636587A Pending JPS63214345A (en) 1987-02-27 1987-02-27 Plasma processing apparatus

Country Status (1)

Country Link
JP (1) JPS63214345A (en)

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