JPH0221296B2 - - Google Patents
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- Publication number
- JPH0221296B2 JPH0221296B2 JP61021795A JP2179586A JPH0221296B2 JP H0221296 B2 JPH0221296 B2 JP H0221296B2 JP 61021795 A JP61021795 A JP 61021795A JP 2179586 A JP2179586 A JP 2179586A JP H0221296 B2 JPH0221296 B2 JP H0221296B2
- Authority
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- Prior art keywords
- plasma
- processing
- magnetic field
- gas
- cylindrical body
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 238000012545 processing Methods 0.000 claims description 37
- 150000002500 ions Chemical class 0.000 claims description 14
- 239000000463 material Substances 0.000 claims description 12
- 239000000843 powder Substances 0.000 claims description 8
- 230000005469 synchrotron radiation Effects 0.000 claims description 7
- BSYNRYMUTXBXSQ-UHFFFAOYSA-N Aspirin Chemical compound CC(=O)OC1=CC=CC=C1C(O)=O BSYNRYMUTXBXSQ-UHFFFAOYSA-N 0.000 claims description 6
- 238000011282 treatment Methods 0.000 claims description 5
- 239000011810 insulating material Substances 0.000 claims description 3
- 241000269627 Amphiuma means Species 0.000 claims 1
- 239000007789 gas Substances 0.000 description 26
- 239000000758 substrate Substances 0.000 description 23
- 238000004381 surface treatment Methods 0.000 description 7
- 238000000034 method Methods 0.000 description 6
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 4
- 230000001133 acceleration Effects 0.000 description 4
- 229910052786 argon Inorganic materials 0.000 description 3
- 238000001816 cooling Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000005530 etching Methods 0.000 description 3
- 239000010408 film Substances 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 239000012212 insulator Substances 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000002245 particle Substances 0.000 description 2
- 239000012495 reaction gas Substances 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 239000010409 thin film Substances 0.000 description 2
- 108010014691 Lithostathine Proteins 0.000 description 1
- 102100027361 Lithostathine-1-alpha Human genes 0.000 description 1
- 229910004298 SiO 2 Inorganic materials 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 238000004140 cleaning Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 239000010410 layer Substances 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000001681 protective effect Effects 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
- 238000000992 sputter etching Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 238000000427 thin-film deposition Methods 0.000 description 1
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B01—PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
- B01J—CHEMICAL OR PHYSICAL PROCESSES, e.g. CATALYSIS OR COLLOID CHEMISTRY; THEIR RELEVANT APPARATUS
- B01J19/00—Chemical, physical or physico-chemical processes in general; Their relevant apparatus
- B01J19/08—Processes employing the direct application of electric or wave energy, or particle radiation; Apparatus therefor
- B01J19/087—Processes employing the direct application of electric or wave energy, or particle radiation; Apparatus therefor employing electric or magnetic energy
- B01J19/088—Processes employing the direct application of electric or wave energy, or particle radiation; Apparatus therefor employing electric or magnetic energy giving rise to electric discharges
Landscapes
- Chemical & Material Sciences (AREA)
- Plasma Technology (AREA)
- Toxicology (AREA)
- General Health & Medical Sciences (AREA)
- Organic Chemistry (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Health & Medical Sciences (AREA)
- Treatments Of Macromolecular Shaped Articles (AREA)
- Inorganic Compounds Of Heavy Metals (AREA)
- Physical Or Chemical Processes And Apparatus (AREA)
- Compounds Of Alkaline-Earth Elements, Aluminum Or Rare-Earth Metals (AREA)
- Carbon And Carbon Compounds (AREA)
- ing And Chemical Polishing (AREA)
- Chemical Vapour Deposition (AREA)
Description
(産業上の利用分野)
本発明は、気体の放電により発生するプラズマ
の活性種、イオン、放射光を処理用材として利用
し、所定の粉体を製造し、又は、被処理基板表面
にエツチング、デポジシヨン、改質、清浄化等の
表面処理を施す放電反応装置に関する。
(従来技術とその問題点)
従来、上記の種類の放電反応装置で最も多く使
用されているものは、第3図に概略の断面を示す
ような平行平板型の表面処理装置である。この装
置では、ガス導入系30と排気系39をそなえる
真空容器31内に対向設置された平行平板型電極
32,33(33は接地された真空容器31に接
続)間に、電源35から直流、交流、高周波など
の電圧を印加して放電を発生させ、その放電プラ
ズマ38を用いて、ヒーター36で加熱される電
極33上の被処理基板37に表面処理を施すもの
である。34は絶縁物である。
同類の装置には、平行平板型電極を同軸円筒型
電極に変形・置換したり、電極数を増減したりし
た様々の装置がある。しかしこれらの装置には共
通して、放電プラズマ38の密度が低く、高速の
処理ができない欠点がある。
また、被処理基板37が放電プラズマ38に直
接接触しているため、荷電粒子の照射を受けて基
板が損傷するという問題もある。この基板の照射
損傷を避けるため、放電プラズマを基板から離れ
た場所で作り、プラズマ中の活性種又はイオンだ
けを被処理基板表面に輸送して処理を行なう装置
も種々提供されているが、何れの装置も放電プラ
ズマの密度がかなり低いために、実用に耐える処
理速度を得るには大電力の投入を必要とする等の
欠点を残している。
なお、プラズマの密度が低いことと、使用する
圧力領域が低いことにより、上記した各装置は粉
体の製造には適しない。
高密度の放電プラズマが得られて、処理速度の
速い、粉体の製造にも利用できる放電反応装置と
しては、第4図に概要の断面を略示するような、
電子サイクロトロン共鳴(ECRと略す)を利用
する放電反応装置がある。この装置を説明する
と、プラズマ発生用ガス導入系42が接続されマ
グネツトコイル40の作る磁場Bの中に設けられ
たプラズマ室41内に、例えば2.45GHzのマイク
ロ波43が投入されると、ECR放電によつて導
入ガスのプラズマが発生する。このプラズマは前
記の磁界Bの下端に作られる発散磁界によつてプ
ラズマ流44となつて処理室45内に拡大および
加速されて噴出し、(必要のときは、ガス導入用
リング状管46を経由して処理室45内に反応用
ガスが導入され、これと協力して)試料台50上
の被処理基板47に所定の処理を施すものであ
る。処理室45には排気系49、プラズマ室41
には冷却系48が接続されている。
しかしこの装置は高密度プラズマとは言つて
も、プラズマ密度が1011cm-3程度であり、イオン
化効率も数%であつてなお低く、そのため大電力
のマイクロ波発振器を必要として、装置が大掛り
で高価になるほか、放電室の形状がECRに適す
る特殊形状に限定されるなどの欠点をもつてい
る。
(発明の目的)
本発明は、上記の問題を解決し、大電力を必要
とせず高効率で高密度のプラズマを生成し、その
プラズマを利用して、経済的に粉体を製造し、ま
たは損傷の少ない高品質の表面処理を高速に行な
うことのできる、小型かつ安価な放電反応装置の
提供を目的とする。
(発明の構成)
本発明は、
(1)a 絶縁物よりなる中空構造の筒状体の内部に
所定のガスを導入する手段、
b 前記筒状体の内部空間に、その軸方向に向
う磁場を形成する手段、
c 前記筒状体の内部空間に、前記軸方向の所
定長さに亙つて、この軸と交わる方向の高周
波交番磁界を印加することにより、磁場中の
定在プラズマ波を用いて該空間内にプラズマ
を発生させる手段、
d 該空間内の該プラズマの活性種、イオン、
放射光を処理用材として、その一部又は全部
を、前記筒状体から処理室に導入する手段、
をそなえ、該導入された該処理用材を用い、若く
は、これに該処理室に別途導入されたガスを加味
して、該処理室内で所定の粉体を生成するか、若
くは、該処理室々内に設置された被処理物の表面
に所定の処理を施す放電反応装置によつて、前記
目的を達成したものである。
(実施例)
以下、図に基いて本発明の放電反応装置の実施
例を説明する。第1図は本発明の実施例の表面処
理装置の概略の断面図であつて、装置は大別して
プラズマ発生部1、処理用材導入部2、処理部3
の3部からなる。
プラズマ発生部1にては、ガラス、石英、石英
ガラス、各種セラミクス等の高融点絶縁材料で作
られた円筒10(必要に応じて、冷却系を付設す
ることがある)内には、図示しないガス供給装置
からバルブ11を通して放電用ガス12が導入さ
れ、円筒10を包囲するコイル13(131,1
32に分割設置されている)には図示しない直流
電源から直流電流が流されて、円筒10の軸方向
に、矢印で図示する磁場B(磁束密度もBとする)
が形成されている。
磁場Bの作成手段として、前記電磁コイルを用
いた場合のみならず、永久磁石を用いても良い
し、永久磁石と電磁コイルを併用しても良い。
更にこの円筒10(直径D)には、その表面に
沿つて軸方向の所定長さ(l)に亘つて、図の如
く特殊な形状に曲折されたアンテナ14が設けら
れ、高周波電源15から整合回路16を経由して
高周波電圧が(周波数、電力W)が印加され
て、円筒10の中に、前記の磁場Bと直交する方
向に、高周波交番磁界が加えられるようになつて
いる。
周知のように、(参考文献。PHYSICS
LETTERS Vol.33A、No.7.P457−P458、
「PLASMA PRODUCTION USING A
STANDING HELICON WAVE(定在ヘリコン
波を用いたプラズマ生成)」14 December1970お
よび、同Vol.91A、No.4.P163−P166、「SOME
FEATURES OF RFEXCITED
FULLYIONIZED LOW PRESSURE ARGON
PLASMA(RFにより励起された低圧完全電離ア
ルゴンプラズマの特性)」6 September1982)、
放電用ガス12をバルブ11を通して導入して後
述のガス排気バルブ25から排気を行ない、円筒
10内のガス圧力を所定値に保ち、アンテナ14
に高周波電力を印加するときは、条件l=(Ba/
nf)0.5によつて、放電管10内のプラズマに定在
プラズマ波の1つであるところの低周波共振とし
ての定在ヘリコン波モードを発生させることがで
きる。但し、aはプラズマの直径、nはプラズマ
の電子密度、l、B、fは前述の通りである。
(放電管内に定在プラズマ波を励起してプラズ
マ中のイオンを共鳴的に加熱することにより、放
電管内に効率的に高密度のプラズマを生起させる
ことの可能な定在プラズマ波としては、ICRF
(Ion Cycrotron Range Frequency)、LH
{Lower Hybrid波(低域混成波)}、Alfven波等
も考えられるが、こゝでは定在Helicon波で代表
させて説明している。)
この条件下では、プラズマ中を電磁波が効果的
に伝搬するため、装置の設計諸元を適当にするこ
とで、現在広く使用されている13.56MHz近辺の
工業用周波数の、比較的小容量の高周波電源を用
いて、極めて効率的に円筒10内にプラズマ密度
が1012cm-3程度以上の高密度のプラズマを発生さ
せることができる。しかも条件によつては放電用
ガスの殆んど100%をイオン化することが可能で
あつて、これはECRプラズマ装置の10倍以上と
いう高い値である。プラズマが高密度であるた
め、生成する活性種、イオンの量は極めて大き
く、放射される光も強大である。
高密度プラズマの高い温度が円筒10を破壊す
るおそれがあり、そのときは、投入する高周波電
力を減じ、若くは、高周波電力をパルス状に断続
的に印加して保護する。
またコイル13に印加する電流をパルス状にし
たり交番状にしたりしても同様の保護作用があ
る。
高密度プラズマの活性種、イオン、放射光等の
処理用材の、一部または全部を処理部3に導入す
る処理用材導入部2は、最も単純には素通りの
まゝにすることもあるが、第1図に示すように、
こゝに金網17、導電性グリツド、絞り等の一層
または多層を設けて、その各層に、浮遊電位、接
地電位、正・負極性の高低の電位を割当てること
で、前記処理用材を選択したり、通過量を適当に
し加速を加減したりして処理室20内に導入す
る。なお、この金網等を、処理室20内に深く侵
入させて基体ホルダー23上の基体24に可成り
近接した位置に置かれることもある。
また放射光のみを利用する場合には光学窓を設
置してもよい。
頭記したECRプラズマ装置では、磁場Bがこ
の処理用材導入部2またはその下方19に作る発
散磁界を利用して、イオン流の幅の拡大と、独自
の調整された加速とを行いうる利点があつたが、
本発明の装置では、電子の運動エネルギーが充分
に大きいので、これに類似する作用を同様の発散
磁界に期待することができる。また前記した処理
室20内に深く侵入させた金網、グリツド等は、
これを上記の発散磁界で拡大されたイオン流の下
方に設置し、これによつてイオン加速の調節の自
由度を高めることもある。かゝる装置は、殊に基
体24の処理がスパツタイオンエツチング処理で
イオンの加速を調節する必要のあるときなどに有
用である。
処理室20に接続される排気系は、排気ポンプ
(図示しない)、排気バルブ25等すべて第3,4
図の従来の場合と同様であつて、処理の種類に適
合したものが使用される。被処理物である基体2
4を加熱ないし冷却するための温度調節系22に
ついても同様である。
基体ホルダー23を回転ないし移動させて、処
理が基体24上で均一になるよう配慮することも
従来と同様である。
さて、基板の処理が単純なエツチングや、Si基
板表面のSiO2皮膜作りあるいは基板表面の有機
物除去等の場合なら、第1図の装置に放電用ガス
12としてArやO2を使用しただけのもので充分
であるが、一層複雑な処理が要求されるときには
第2図の実施例(概要の断面図で示す)のよう
な、処理用ガス28を導入加味する放電反応装置
が有利である。
図示しないガス供給装置から供給される処理用
ガス28は、バルブ27を経由してガス導入用リ
ング状管26に入り、リング状管26のリング内
側に多数穿設されたガス噴出孔260から央部に
向つて基板24の表面上に噴出し、円筒10から
処理室20へと導入された前述の活性種、イオ
ン、放射光の一部または全部の照射をうけて、そ
れらのエネルギーにより反応を起し、基板24の
表面に、薄膜堆積などの所定の処理を施すことに
なる。
第1表に、堆積できる薄膜の種類と、そのとき
利用される放電用ガス、処理用ガスの組合せを例
示した。
処理用材導入部2と処理部3の構成を適当に選
ぶときは、これら多種類の薄膜を、膜質、膜厚の
分布を均一にし、かつ荷電粒子の照射衝撃による
損傷を避けながら、基板24上に高速に堆積させ
ることができる。
なお、例えばECRのように電子の共鳴により
高密度プラズマを得る場合には、電子の平均自由
行程が、そのラーマー半径に比べて十分大きいこ
とが必要であり、ガス圧力をある程度以上あげる
ことはできないが、定在プラズマ波例えば定在ヘ
リコン波によつてプラズマを発生させる場合はガ
ス圧力を上げて、高密度状態で反応を進行させる
ことが可能であり、第1表の左欄の各物質の粉体
を作成することも容易である。この場合は圧力を
上昇させると有効である。
(Industrial Application Field) The present invention utilizes plasma active species, ions, and synchrotron radiation generated by gas discharge as processing materials to produce a predetermined powder, or to perform etching and etching on the surface of a substrate to be processed. This invention relates to a discharge reactor that performs surface treatments such as deposition, modification, and cleaning. (Prior Art and its Problems) Conventionally, the most commonly used discharge reaction apparatus of the above type is a parallel plate type surface treatment apparatus, a schematic cross section of which is shown in FIG. In this device, direct current is supplied from a power source 35 between parallel plate electrodes 32 and 33 (33 is connected to the grounded vacuum vessel 31), which are placed opposite each other in a vacuum vessel 31 having a gas introduction system 30 and an exhaust system 39. A voltage such as an alternating current or high frequency voltage is applied to generate a discharge, and the discharge plasma 38 is used to perform surface treatment on the substrate 37 to be processed on the electrode 33 heated by the heater 36. 34 is an insulator. Similar devices include various devices in which parallel plate electrodes are modified or replaced with coaxial cylindrical electrodes, or the number of electrodes is increased or decreased. However, these devices have a common drawback that the discharge plasma 38 has a low density and cannot perform high-speed processing. Further, since the substrate 37 to be processed is in direct contact with the discharge plasma 38, there is a problem that the substrate is damaged by being irradiated with charged particles. In order to avoid radiation damage to the substrate, various devices have been proposed that generate discharge plasma at a location away from the substrate and transport only the active species or ions in the plasma to the surface of the substrate to be processed. This device also has drawbacks, such as requiring a large amount of power to obtain a processing speed suitable for practical use because the density of the discharge plasma is quite low. Note that each of the above-mentioned apparatuses is not suitable for producing powder due to the low density of plasma and the low pressure range used. A discharge reactor that can obtain high-density discharge plasma, has a high processing speed, and can also be used for powder production is the one whose cross section is schematically shown in Figure 4.
There is a discharge reactor that utilizes electron cyclotron resonance (abbreviated as ECR). To explain this device, when a microwave 43 of, for example, 2.45 GHz is injected into a plasma chamber 41 connected to a plasma generation gas introduction system 42 and provided in a magnetic field B generated by a magnet coil 40, ECR is generated. Plasma of the introduced gas is generated by the discharge. This plasma becomes a plasma flow 44 by the diverging magnetic field created at the lower end of the magnetic field B, and is expanded and accelerated into the processing chamber 45 and ejected (if necessary, the ring-shaped pipe 46 for gas introduction is opened). A reaction gas is introduced into the processing chamber 45 via the reaction chamber 45, and in cooperation with the reaction gas, a predetermined process is performed on the substrate 47 to be processed on the sample stage 50. The processing chamber 45 includes an exhaust system 49 and a plasma chamber 41.
A cooling system 48 is connected to. However, although this device uses high-density plasma, the plasma density is around 10 11 cm -3 , and the ionization efficiency is still low at only a few percent. Therefore, it requires a high-power microwave oscillator, making the device very large. In addition to being expensive, the shape of the discharge chamber is limited to a special shape suitable for ECR. (Objective of the Invention) The present invention solves the above problems, generates high-efficiency and high-density plasma without requiring large electric power, uses the plasma to economically produce powder, or The purpose of the present invention is to provide a small and inexpensive discharge reaction device that can perform high-quality surface treatment with little damage at high speed. (Structure of the Invention) The present invention provides: (1)a means for introducing a predetermined gas into the interior of a hollow cylindrical body made of an insulating material; b a magnetic field directed in the axial direction of the internal space of the cylindrical body; c) applying a high-frequency alternating magnetic field in a direction intersecting the axis over a predetermined length in the axial direction to the internal space of the cylindrical body, using a standing plasma wave in the magnetic field; means for generating plasma in the space; d. active species, ions of the plasma in the space;
A means for introducing synchrotron radiation as a processing material, in part or in its entirety, from the cylindrical body into the processing chamber; A predetermined powder is generated in the processing chamber by taking into account the gas produced, or, more recently, by an electric discharge reaction device that performs a predetermined treatment on the surface of the object to be treated, which is installed in the processing chambers. , the above objective has been achieved. (Example) Hereinafter, an example of the discharge reaction device of the present invention will be described based on the drawings. FIG. 1 is a schematic cross-sectional view of a surface treatment apparatus according to an embodiment of the present invention, and the apparatus is roughly divided into a plasma generation section 1, a treatment material introduction section 2, and a treatment section 3.
It consists of three parts. In the plasma generation section 1, a cylinder 10 (not shown) made of a high melting point insulating material such as glass, quartz, quartz glass, various ceramics, etc. (a cooling system may be attached as necessary) is provided. A discharge gas 12 is introduced from a gas supply device through a valve 11, and a coil 13 (131, 1
A DC current is passed from a DC power supply (not shown) through the cylinder 10 (separated into 32 sections), and a magnetic field B (magnetic flux density is also assumed to be B) is generated in the axial direction of the cylinder 10, as shown by the arrow.
is formed. As means for creating the magnetic field B, not only the electromagnetic coil described above may be used, but a permanent magnet may be used, or a permanent magnet and an electromagnetic coil may be used in combination. Further, this cylinder 10 (diameter D) is provided with an antenna 14 bent into a special shape as shown in the figure over a predetermined length (l) in the axial direction along its surface, and receives a matching signal from a high frequency power source 15. A high frequency voltage (frequency, power W) is applied via the circuit 16, and a high frequency alternating magnetic field is applied inside the cylinder 10 in a direction orthogonal to the magnetic field B described above. As is well known, (References. PHYSICS
LETTERS Vol.33A, No.7.P457−P458,
“PLASMA PRODUCTION USING A
STANDING HELICON WAVE (Plasma generation using standing helicon waves)” 14 December 1970 and the same Vol.91A, No.4.P163-P166, “SOME
FEATURES OF RFEXCITED
FULLYIONIZED LOW PRESSURE ARGON
PLASMA (Characteristics of low-pressure fully ionized argon plasma excited by RF)” 6 September 1982),
The discharge gas 12 is introduced through the valve 11 and exhausted from a gas exhaust valve 25 (described later) to maintain the gas pressure inside the cylinder 10 at a predetermined value, and the antenna 14 is
When applying high frequency power to
nf) 0.5 , it is possible to generate a standing helicon wave mode as a low frequency resonance, which is one of the standing plasma waves, in the plasma in the discharge tube 10. However, a is the diameter of the plasma, n is the electron density of the plasma, and l, B, and f are as described above. (ICRF is a standing plasma wave that can efficiently generate high-density plasma inside a discharge tube by exciting the standing plasma wave inside the discharge tube and resonantly heating the ions in the plasma.)
(Ion Cyclotron Range Frequency), LH
{Lower Hybrid waves}, Alfven waves, etc. are also possible, but here we will use standing Helicon waves as a representative. ) Under these conditions, electromagnetic waves propagate effectively in the plasma, so by appropriate design specifications of the equipment, relatively small-capacity High-density plasma with a plasma density of about 10 12 cm -3 or more can be generated extremely efficiently in the cylinder 10 using a high-frequency power source. Furthermore, depending on the conditions, it is possible to ionize almost 100% of the discharge gas, which is more than 10 times higher than that of an ECR plasma device. Since plasma is highly dense, the amount of active species and ions produced is extremely large, and the emitted light is also powerful. There is a risk that the high temperature of the high-density plasma may destroy the cylinder 10, and in that case, the input high-frequency power should be reduced, or in the future, the high-frequency power should be applied intermittently in a pulsed manner to protect it. Further, the same protective effect can be obtained even if the current applied to the coil 13 is pulsed or alternated. The processing material introducing section 2, which introduces some or all of the processing materials such as active species of high-density plasma, ions, and synchrotron radiation into the processing section 3, may be left as it is in the simplest case. As shown in Figure 1,
By providing a single layer or multiple layers such as a wire mesh 17, conductive grid, orifice, and assigning a floating potential, a ground potential, and potentials of high and low positive and negative polarity to each layer, the material to be treated can be selected. , and introduce it into the processing chamber 20 by adjusting the amount of passage and adjusting the acceleration. Note that this wire mesh or the like may be deeply penetrated into the processing chamber 20 and placed at a position quite close to the substrate 24 on the substrate holder 23. Furthermore, if only synchrotron radiation is used, an optical window may be installed. The above-mentioned ECR plasma apparatus has the advantage that the width of the ion flow can be expanded and uniquely adjusted acceleration can be performed by utilizing the diverging magnetic field created by the magnetic field B in the processing material introduction part 2 or its lower part 19. It was hot, but
In the device of the present invention, since the kinetic energy of electrons is sufficiently large, a similar effect can be expected from a similar divergent magnetic field. In addition, the wire mesh, grid, etc. that have penetrated deeply into the processing chamber 20 described above,
This may be installed below the ion flow expanded by the above-mentioned divergent magnetic field, thereby increasing the degree of freedom in adjusting ion acceleration. Such an apparatus is particularly useful when processing the substrate 24 in a sputter ion etching process in which ion acceleration needs to be controlled. The exhaust system connected to the processing chamber 20 includes an exhaust pump (not shown), an exhaust valve 25, etc.
Similar to the conventional case shown in the figure, a method suitable for the type of processing is used. Substrate 2 which is the object to be processed
The same applies to the temperature control system 22 for heating or cooling the air conditioner 4. Similarly to the conventional method, consideration is given to rotating or moving the substrate holder 23 so that the processing is uniform on the substrate 24. Now, if the processing of the substrate is simple etching, the creation of a SiO 2 film on the surface of a Si substrate, or the removal of organic substances from the surface of a substrate, it is possible to use the apparatus shown in Fig. 1 by simply using Ar or O 2 as the discharge gas 12. However, when a more complex process is required, a discharge reactor, such as the embodiment shown in FIG. 2 (shown in a schematic cross-sectional view), which incorporates a process gas 28, is advantageous. The processing gas 28 supplied from a gas supply device (not shown) enters the gas introduction ring-shaped pipe 26 via the valve 27, and enters the ring-shaped pipe 26 from a large number of gas ejection holes 260 bored inside the ring of the ring-shaped pipe 26. The active species, ions, and synchrotron radiation emitted from the cylinder 10 into the processing chamber 20 are ejected onto the surface of the substrate 24 toward the surface of the substrate 24, and are irradiated with some or all of the above-mentioned active species, ions, and synchrotron radiation, and undergo a reaction due to their energy. Then, a predetermined process such as thin film deposition is performed on the surface of the substrate 24. Table 1 lists examples of the types of thin films that can be deposited and the combinations of discharge gas and processing gas used at that time. When appropriately selecting the configurations of the processing material introducing section 2 and the processing section 3, these various types of thin films can be deposited on the substrate 24 while making the film quality and thickness distribution uniform and avoiding damage caused by the irradiation impact of charged particles. can be deposited at high speed. Note that when obtaining high-density plasma through electron resonance, as in ECR, for example, the mean free path of the electrons must be sufficiently large compared to the Larmor radius, and the gas pressure cannot be increased beyond a certain level. However, when plasma is generated by a standing plasma wave, such as a standing helicon wave, it is possible to increase the gas pressure and allow the reaction to proceed in a high density state. It is also easy to create powder. In this case, it is effective to increase the pressure.
【表】【table】
【表】
(発明の効果)
本発明は、高効率で生成される高密度のプラズ
マにより、経済的に粉体を製造し、または、損傷
の少ない高品質の表面処理を高速に行なうことの
できる小型かつ安価な放電反応装置を提供する効
果がある。[Table] (Effects of the invention) The present invention makes it possible to economically produce powder or perform high-quality surface treatment with little damage at high speed using high-density plasma generated with high efficiency. This has the effect of providing a small and inexpensive discharge reactor.
第1図は、本発明の実施例の放電反応装置の概
略の断面図。第2図は、別の実施例の同様の図。
第3図は、従来の平行平板型表面処理装置の概略
の断面図。第4図は、従来のECRプラズマ装置
の概略の断面図。
1……プラズマ発生部、2……処理用材導入
部、3……処理部、10……絶縁物よりなる円
筒、11……放電用ガス12の導入用バルブ、1
3……電磁コイル、14……アンテナ、15……
高周波電源、16……整合回路、17……金網、
20……処理室、22……温度調節系、23……
基板ホルダー、24……基板、25……排気バル
ブ、26……ガス導入用リング状管、27……処
理用ガス28の導入用バルブ。
FIG. 1 is a schematic sectional view of a discharge reactor according to an embodiment of the present invention. FIG. 2 is a similar diagram of another embodiment.
FIG. 3 is a schematic cross-sectional view of a conventional parallel plate type surface treatment apparatus. FIG. 4 is a schematic cross-sectional view of a conventional ECR plasma device. DESCRIPTION OF SYMBOLS 1...Plasma generation part, 2...Processing material introduction part, 3...Processing part, 10...Cylinder made of an insulator, 11...Valve for introducing discharge gas 12, 1
3... Electromagnetic coil, 14... Antenna, 15...
High frequency power supply, 16... matching circuit, 17... wire mesh,
20...Processing chamber, 22...Temperature control system, 23...
Substrate holder, 24...Substrate, 25...Exhaust valve, 26...Ring-shaped pipe for introducing gas, 27...Valve for introducing processing gas 28.
Claims (1)
に所定のガスを導入する手段、 b 前記筒状体の内部空間に、その軸方向に向う
磁場を形成する手段、 c 前記筒状体の内部空間に、前記軸方向の所定
長さに亙つて、この軸と交わる方向の高周波交
番磁界を印加することにより、磁場中の定在プ
ラズマ波を用いて該空間内にプラズマを発生さ
せる手段、 d 該空間内の該プラズマの活性種、イオン、放
射光を処理用材として、その一部又は全部を、
前記筒状体から処理室に導入する手段、 をそなえ、 該導入された処理用材を用い、若くは、これに
該処理室に別途導入されたガスを加味することに
よつて、該処理室内で所定の粉体を生成するか、
若くは、該処理室々内に設置された被処理物の表
面に所定の処理を施すことを特徴とする放電反応
装置。 2 定在プラズマ波が定在ヘリコン波である特許
請求の範囲第1項記載の放電反応装置。[Scope of Claims] 1 a. Means for introducing a predetermined gas into the interior of a hollow cylindrical body made of an insulating material; b. Means for forming a magnetic field in the internal space of the cylindrical body in the axial direction thereof; c. By applying a high-frequency alternating magnetic field in a direction intersecting the axis over a predetermined length in the axial direction to the internal space of the cylindrical body, a standing plasma wave in the magnetic field is used to generate energy within the space. means for generating plasma; d. using active species, ions, and synchrotron radiation of the plasma in the space as processing materials, part or all of which;
means for introducing the processing material from the cylindrical body into the processing chamber, and using the introduced processing material, or by adding a gas separately introduced into the processing chamber, Generate a given powder or
A discharge reaction device is characterized in that it performs a predetermined treatment on the surface of an object to be treated installed in the treatment chambers. 2. The discharge reaction device according to claim 1, wherein the standing plasma wave is a standing helicon wave.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61021795A JPS62180747A (en) | 1986-02-03 | 1986-02-03 | Electric discharge reaction device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61021795A JPS62180747A (en) | 1986-02-03 | 1986-02-03 | Electric discharge reaction device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62180747A JPS62180747A (en) | 1987-08-08 |
| JPH0221296B2 true JPH0221296B2 (en) | 1990-05-14 |
Family
ID=12064987
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61021795A Granted JPS62180747A (en) | 1986-02-03 | 1986-02-03 | Electric discharge reaction device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62180747A (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO1995008182A1 (en) * | 1993-09-17 | 1995-03-23 | Isis Innovation Limited | Rf plasma reactor |
| JPH07142463A (en) * | 1993-11-22 | 1995-06-02 | Nec Corp | Method and equipment for fabricating semiconductor device |
| SE521904C2 (en) * | 1999-11-26 | 2003-12-16 | Ladislav Bardos | Hybrid Plasma Treatment Device |
| JP2012130825A (en) * | 2010-12-20 | 2012-07-12 | Kagawa Univ | Nano-particle manufacturing method, nano-particles, and nano-particle manufacturing apparatus |
| JP6055721B2 (en) * | 2013-05-31 | 2016-12-27 | フルード工業株式会社 | Powder physical property measuring device |
-
1986
- 1986-02-03 JP JP61021795A patent/JPS62180747A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62180747A (en) | 1987-08-08 |
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