JPS6380523A - Microwave plasma processing equipment - Google Patents
Microwave plasma processing equipmentInfo
- Publication number
- JPS6380523A JPS6380523A JP61225246A JP22524686A JPS6380523A JP S6380523 A JPS6380523 A JP S6380523A JP 61225246 A JP61225246 A JP 61225246A JP 22524686 A JP22524686 A JP 22524686A JP S6380523 A JPS6380523 A JP S6380523A
- Authority
- JP
- Japan
- Prior art keywords
- plasma processing
- microwave
- microwave plasma
- cylindrical
- processing apparatus
- 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
Links
Landscapes
- Drying Of Semiconductors (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) [Abstract] 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
本発明は半導体プロセス技術2表面処理技術等において
、マイクロ波により発生させたプラズマにより、膜付け
、エツチング等の薄膜処理をするためのマイクロ波プラ
ズマ処理装置に関し、特に高密度プラズマにより高速の
薄膜処理を実現する装置を提供するものである。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to semiconductor process technology 2, surface treatment technology, etc., and is directed to microwave plasma processing for thin film processing such as film deposition and etching using plasma generated by microwaves. In particular, the present invention provides an apparatus that realizes high-speed thin film processing using high-density plasma.
従来の技術
従来のマイクロ波プラズマ処理装置は、例えば特開昭5
8−125820号公報に示されているように第3図の
ような構造になっていた。2. Description of the Related Art A conventional microwave plasma processing apparatus is, for example, disclosed in Japanese Patent Application Laid-open No. 5
As shown in Japanese Patent No. 8-125820, it had a structure as shown in FIG.
すなわちマイクロ波1が導波管2から、円筒導波管3に
テーパ導波管4を経て導入される。その際、真空を保ち
、マイクロ波は損失なく導入されるだめの石英板5が設
けられている。そしてこの円筒導波管3の外部に配置さ
れたコバルトサマリウム(Sm−Co)磁石6が真空室
7に、周波数2.45GH2のマイクロ波に対して、8
75ガウスの磁場が存在し、ガス導入口8から、例えば
シラン(S 1H4) ガスを導入すると、ECR放
電を生じる。その中に回転手段9から回転が導入された
支持台10の上に感光用ドラム11を設けると、例えば
感光用ドラム11にa−3i を堆積させることができ
る。That is, the microwave 1 is introduced from the waveguide 2 into the cylindrical waveguide 3 via the tapered waveguide 4. At this time, a quartz plate 5 is provided to maintain a vacuum and allow microwaves to be introduced without loss. A cobalt samarium (Sm-Co) magnet 6 placed outside the cylindrical waveguide 3 is placed in the vacuum chamber 7 to generate a microwave with a frequency of 2.45 GH2.
A magnetic field of 75 Gauss exists, and when a silane (S 1H4) gas, for example, is introduced through the gas inlet 8, an ECR discharge occurs. If the photosensitive drum 11 is provided on a support base 10 into which rotation is introduced from the rotating means 9, a-3i can be deposited on the photosensitive drum 11, for example.
発明が解決しようとする問題点
しかし、このような構造のものでは感光用ドラム台12
がマイクロ波に対して障害物となり、反射波が多くなる
ために、マイクロ波電力が効率よくプラズマに吸収され
ない。また、磁石6による磁場は円筒導波管3の周辺で
しかECR条件を満足できないために、感光用ドラム台
12を反射波が少くなるような大きさにするとプラズマ
の拡散領域が大きくなυ高密度のプラズマを感光用ドラ
ム11の近傍に生成することができなかった。Problems to be Solved by the Invention However, with such a structure, the photosensitive drum stand 12
becomes an obstacle to the microwaves, and the number of reflected waves increases, so the microwave power is not efficiently absorbed by the plasma. Furthermore, since the magnetic field generated by the magnet 6 can only satisfy the ECR conditions around the cylindrical waveguide 3, if the photosensitive drum stand 12 is made to a size that reduces reflected waves, the plasma diffusion area will be large and the υ height will be increased. It was not possible to generate dense plasma near the photosensitive drum 11.
問題点を解決するための手段
そして上記問題点を解決する本発明の技術的な手段は、
マイクロ波のプラズマ生成室への導入には円筒状アンテ
ナを用い、試料を保持するための筒体の内部から永久磁
石で円筒状アンテナの内部にECR条件を満足させる磁
場を発生させるものである。Means for solving the problems and technical means of the present invention for solving the above problems are as follows:
A cylindrical antenna is used to introduce microwaves into the plasma generation chamber, and a permanent magnet is used from inside the cylindrical body for holding the sample to generate a magnetic field inside the cylindrical antenna that satisfies the ECR conditions.
作 用 この技術的手段による作用は次のようになる。For production The effect of this technical means is as follows.
すなわち、円筒状アンテナにより放射されるマイクロ波
電力は試料を保持するための筒体の形状には関係なく、
円筒状アンテナ内部でプラズマを生成するために必要な
電界を発生させる。まだ、試料保持用筒体内部に設けら
れた磁界印加手段により試料表面に強い磁界を発生させ
ることができ、これがECR条件を満足する磁界になれ
ば、ECR放電を起こすものである。In other words, the microwave power radiated by the cylindrical antenna is independent of the shape of the cylinder used to hold the sample.
Generate the electric field necessary to generate plasma inside the cylindrical antenna. Still, a strong magnetic field can be generated on the sample surface by the magnetic field applying means provided inside the sample holding cylinder, and if this magnetic field satisfies the ECR conditions, ECR discharge will occur.
実施例
以下、本発明の一実施例を添付図面にもとづいて説明す
る。Embodiment Hereinafter, one embodiment of the present invention will be described based on the accompanying drawings.
第1図および第2図において、21は真空室であり、ガ
ス導入口22とマイクロ波導入口23とを有している。In FIGS. 1 and 2, 21 is a vacuum chamber, which has a gas inlet 22 and a microwave inlet 23. In FIG.
真空室21内にはマイクロ波放射用アンテナであるスロ
ッテッドライン型のヘリカルコイル、通称リジタノコイ
ル24が設けである。A slotted line type helical coil, commonly known as a rigid coil 24, which is a microwave radiation antenna, is provided in the vacuum chamber 21.
リジタノコイル24の内部には非磁性体の筒体25が固
定されており、その内周には磁界印加手段としての複数
の棒状の磁石体26(たとえば、コバルトサマリウム系
の永久磁石)を筒体26の周方向に沿って配列して、筒
体25の壁面に対面した磁極が交互にN極・S極になる
ようにしてあり、リジタノコイル24と筒体25の間に
磁力線27を発生させる。また、筒体25の壁面に対面
した磁極と反対側の磁極は磁性体でできた環状ヨーク2
日に接してお9、磁気回路を形成している。筒体25に
は冷却パイプ29が取り付けてあり、磁石体26が冷却
できるようになっている。A non-magnetic cylinder 25 is fixed inside the rigid coil 24, and a plurality of rod-shaped magnets 26 (for example, cobalt samarium-based permanent magnets) are attached to the inner circumference of the cylinder 25. The magnetic poles facing the wall surface of the cylindrical body 25 are arranged along the circumferential direction so that the magnetic poles facing the wall surface of the cylindrical body 25 alternately become N poles and S poles, and generate lines of magnetic force 27 between the rigid coil 24 and the cylindrical body 25. In addition, the magnetic pole facing the wall surface of the cylinder 25 and the magnetic pole on the opposite side are an annular yoke 2 made of a magnetic material.
When exposed to the sun, it forms a magnetic circuit. A cooling pipe 29 is attached to the cylindrical body 25 so that the magnet body 26 can be cooled.
このような構造において、ガス導入口22を通してアル
ゴンなどの被イオン化ガスを導入する。In such a structure, a gas to be ionized, such as argon, is introduced through the gas inlet 22.
マイクロ波は、たとえば周波数2.45GH2のマグネ
トロン3oなら、300 Wa t tの平均出力を導
波管31を通って、マイクロ波導入口23を経て、リジ
タノコイル24へ導かれる。このとき、磁石体26の漏
れ磁束の密度をリジタノコイル24上で電子サイクロト
ロン共鳴にiるように設定(たとえば2 、45 G
Hzの周波数に対しては875ガウス)すると、リジタ
ノコイル24と筒体25の間に高密度のプラズマが生成
される(参考文献:R9De Dionigi、M、
Fontahesi、 E、5indoni andG
、Li5itano;Applied Physics
Letters、Vol。For example, if the microwave is a magnetron 3o with a frequency of 2.45 GH2, an average output of 300 Watts passes through the waveguide 31, passes through the microwave inlet 23, and is guided to the rigid coil 24. At this time, the density of the leakage magnetic flux of the magnet body 26 is set to reach electron cyclotron resonance on the rigidano coil 24 (for example, 2, 45 G
875 Gauss for a frequency of Hz), a high-density plasma is generated between the rigid coil 24 and the cylinder 25 (Reference: R9De Dionigi, M.
Fontahesi, E., 5indoni and G.
, Li5itano; Applied Physics
Letters, Vol.
19、(1971)、P、19)。筒体25の外周に試
料32を取り付ければ、ガス導入口22からシラン(S
1H4)ガスを導入すると試料32上にa−3iが生
成できる。また、たとえば、筒体25にリジタノコイル
24に対して負電圧を印加すれば、イオンエツチング装
置として利用できる。19, (1971), P, 19). When the sample 32 is attached to the outer periphery of the cylinder 25, silane (S
1H4) When a gas is introduced, a-3i can be generated on the sample 32. Further, for example, if a negative voltage is applied to the cylindrical body 25 with respect to the rigid coil 24, it can be used as an ion etching device.
寸た、本実施例に2いて、リジタノコイル24をらせん
状に切れ目がちるヘリカル型となっているが、切れ目が
軸と垂直であるデジタル型にしても同様の効果を奏する
。また31は導波管となっているが、同軸線にしても同
様の効果を奏する。In the second embodiment, the rigid coil 24 is of a helical type with helical cuts, but the same effect can be obtained even if it is of a digital type with cuts perpendicular to the axis. Moreover, although 31 is a waveguide, the same effect can be obtained even if it is a coaxial line.
発明の効果
本発明は、プラズマ生成のための電力供給手段としてリ
ジタノコイルを用い、ECR条件を満足させるための磁
界を円筒状の試料台の内部から永久磁石により印加する
ことにより、プラズマ密度10 個/adの高密度プラ
ズマを試料近傍に得ることができた。Effects of the Invention The present invention uses a rigid coil as a power supply means for plasma generation, and applies a magnetic field to satisfy ECR conditions from inside a cylindrical sample stage using a permanent magnet, thereby increasing the plasma density to 10 particles/ We were able to obtain high-density ad plasma near the sample.
第1図は本発明の一実施例のマイクロ波プラズマ処理装
置の縦断面図、第2図は同装置のA−A線断面図、第3
図は従来のマイクロ波プラズマ処理装置の縦断面図であ
る。
21・・・・・・真空室、22・・・・・・ガス導入口
、23・・・・・・マイクロ波導入口、24・・・・・
・リジタノコイル(円筒状アンテナ)、25・・・・・
・筒体、26・・・・・・磁石体(磁界印加手段)、3
2・・・・・・試料。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名21
・−真空室
2と一乃′ス捧へ℃
25−一一茄滲
2C−’o’+Q石イ本Ci益Tfull刀ロナにノ3
2−−−言氏料
第2図
第3図FIG. 1 is a longitudinal sectional view of a microwave plasma processing apparatus according to an embodiment of the present invention, FIG. 2 is a sectional view taken along line A-A of the same apparatus, and FIG.
The figure is a longitudinal sectional view of a conventional microwave plasma processing apparatus. 21...Vacuum chamber, 22...Gas inlet, 23...Microwave inlet, 24...
・Rigidano coil (cylindrical antenna), 25...
- Cylindrical body, 26... Magnet body (magnetic field applying means), 3
2... Sample. Name of agent: Patent attorney Toshio Nakao and 1 other person21
・-Vacuum chamber 2 and Ichino's dedicated to ℃ 25-11 茄滲2C-'o'+Q Ishiimoto Ci benefit Tfull sword Rona ni no 3
2---Charge fee Figure 2 Figure 3
Claims (5)
、前記真空室内にマイクロ波を放射するために前記マイ
クロ波導入口と接続された円筒状アンテナと、円筒状ア
ンテナ内に設けられた試料を保持するための筒体と、前
記円筒状アンテナと前記筒体との間に磁界を印加する磁
界印加手段とを備え、前記磁界印加手段は前記筒体の内
側に壁面に沿って配置され壁面に接した隣合う磁極が相
異なる複数の磁石体からなるマイクロ波プラズマ処理装
置。(1) A vacuum chamber having a gas inlet and a microwave inlet, a cylindrical antenna connected to the microwave inlet for radiating microwaves into the vacuum chamber, and a sample provided in the cylindrical antenna. A cylindrical body for holding the antenna, and a magnetic field applying means for applying a magnetic field between the cylindrical antenna and the cylindrical body. A microwave plasma processing device consisting of multiple magnet bodies with different adjacent magnetic poles.
リカルコイル(リジタノコイル)を用いた特許請求の範
囲第1項記載のマイクロ波プラズマ処理装置。(2) The microwave plasma processing apparatus according to claim 1, which uses a slotted line type helical coil (rigidano coil) as the cylindrical antenna.
クロトロン共鳴を起す特許請求の範囲第1項記載のマイ
クロ波プラズマ処理装置。(3) The microwave plasma processing apparatus according to claim 1, wherein the magnetic field causes electron cyclotron resonance with respect to the frequency of the microwave.
る特許請求の範囲第1項記載のマイクロ波プラズマ処理
装置。(4) The microwave plasma processing apparatus according to claim 1, wherein the magnet body is a cobalt samarium-based rare earth magnet.
載のマイクロ波プラズマ処理装置。(5) The microwave plasma processing apparatus according to claim 1, wherein the cylindrical body is provided with a cooling means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61225246A JPS6380523A (en) | 1986-09-24 | 1986-09-24 | Microwave plasma processing equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61225246A JPS6380523A (en) | 1986-09-24 | 1986-09-24 | Microwave plasma processing equipment |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6380523A true JPS6380523A (en) | 1988-04-11 |
Family
ID=16826291
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61225246A Pending JPS6380523A (en) | 1986-09-24 | 1986-09-24 | Microwave plasma processing equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6380523A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0250960A (en) * | 1988-08-12 | 1990-02-20 | Canon Inc | sputtering equipment |
| JPH0379421U (en) * | 1989-12-01 | 1991-08-13 | ||
| US6217661B1 (en) | 1987-04-27 | 2001-04-17 | Semiconductor Energy Laboratory Co., Ltd. | Plasma processing apparatus and method |
-
1986
- 1986-09-24 JP JP61225246A patent/JPS6380523A/en active Pending
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6217661B1 (en) | 1987-04-27 | 2001-04-17 | Semiconductor Energy Laboratory Co., Ltd. | Plasma processing apparatus and method |
| US6423383B1 (en) | 1987-04-27 | 2002-07-23 | Semiconductor Energy Laboratory Co., Ltd. | Plasma processing apparatus and method |
| US6838126B2 (en) | 1987-04-27 | 2005-01-04 | Semiconductor Energy Laboratory Co., Ltd. | Method for forming I-carbon film |
| JPH0250960A (en) * | 1988-08-12 | 1990-02-20 | Canon Inc | sputtering equipment |
| JPH0379421U (en) * | 1989-12-01 | 1991-08-13 |
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