JPH02254170A - Plasma treating device - Google Patents

Plasma treating device

Info

Publication number
JPH02254170A
JPH02254170A JP7394189A JP7394189A JPH02254170A JP H02254170 A JPH02254170 A JP H02254170A JP 7394189 A JP7394189 A JP 7394189A JP 7394189 A JP7394189 A JP 7394189A JP H02254170 A JPH02254170 A JP H02254170A
Authority
JP
Japan
Prior art keywords
coil
sample
plasma
magnetic field
distribution
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.)
Granted
Application number
JP7394189A
Other languages
Japanese (ja)
Other versions
JPH064917B2 (en
Inventor
Mikiho Kiuchi
木内 幹保
Seitaro Matsuo
松尾 誠太郎
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.)
NTT Inc
Original Assignee
Nippon Telegraph and Telephone Corp
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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP7394189A priority Critical patent/JPH064917B2/en
Publication of JPH02254170A publication Critical patent/JPH02254170A/en
Publication of JPH064917B2 publication Critical patent/JPH064917B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To increase the area of a region subjected to treatment and the rate of treatment by fitting a flat coil to the side of a sample stand reverse to the sample holding side in a device for treating a sample by irradiation with plasma generated by utilizing microwaves. CONSTITUTION:Microwaves are introduced into a plasma generation chamber 1, plasma is generated and a sample 11 on a sample stand 10 is treated with a plasma jet 8 led from the chamber 1. A flat coil 15 is fitted to the side of the stand 10 reverse to the sample holding side. The distribution of a magnetic field near the stand 10 is controlled by the coil 15 and a uniform high rate of plasma treatment is obtd.

Description

【発明の詳細な説明】 1産業上の利用分!l!f] 本発明はプラズマおよびそれに含まれるイオンを利用し
て材料表面上に薄膜を形成するために、または材料表面
をエツチングするために用いるプラズマ処理装置に関す
るものであり、特に半導体集積回路などの各種デバイス
の製造工程に適合するプラズマ処理装置に関するもので
ある。
[Detailed description of the invention] 1 industrial use! l! f] The present invention relates to a plasma processing apparatus used for forming a thin film on the surface of a material or etching the surface of a material by using plasma and the ions contained therein, and particularly relates to a plasma processing apparatus used for etching various types of semiconductor integrated circuits. The present invention relates to a plasma processing apparatus that is compatible with device manufacturing processes.

[従来の技術] 薄膜形成およびエツチングに用いるプラズマ生成法とし
て、マイクロ波励起による電子ザイクロトロン共喝を利
用したプラズマ生成法があり、これは低カス圧、高イオ
ン化率、高活性の特(敢を有し、導入ガスの選択、イオ
ンエネルギーの制御によって優れた加工特性を発揮しう
ることが明らかにされている。
[Prior art] As a plasma generation method used for thin film formation and etching, there is a plasma generation method that utilizes electron cyclotron co-pulsation by microwave excitation, which has the characteristics of low gas pressure, high ionization rate, and high activity. It has been revealed that excellent processing characteristics can be exhibited by selecting the introduced gas and controlling the ion energy.

第7図にマイクロ波電子サイクロ1〜ロン共鳴プラズマ
を利用した、従来のプラズマ処理装置の基本構成図を示
す。ここに、1ば、プラズマ生成室、2は試料室、12
は排気路、3はマイクロ波導入窓であって例えは石英ガ
ラス板により構成されている。4はマイクロ波導入のた
めの矩形導波管である。9はプラズマ生成室1で生成さ
れたプラズマを試a合10に載置された試着11に導く
ためのプラズマ引出し窓である。13はプラズマ生成室
1の内部の適当な領域で電子サイクロl−ロン共鴨条件
を満す磁界強度を発生させるための磁気コイルであり、
プラズマ流8を形成させるための発散611界の形成に
も利用している。図示を省略したマイクロ波源は、例え
ば周波数2.45GHzのマグネトロンを用いて構成さ
れる。5はプラズマ生成室の冷却水路、6および7はガ
ス尋人用の第1ガス導入系および第2ガス導入系てあり
、処理目的に応じて、それそわ単独もしくは組合せて使
用する。
FIG. 7 shows a basic configuration diagram of a conventional plasma processing apparatus that utilizes microwave electron cyclo1-ron resonance plasma. Here, 1B is a plasma generation chamber, 2 is a sample chamber, and 12 is a plasma generation chamber.
3 is an exhaust path, and 3 is a microwave introduction window, which is made of, for example, a quartz glass plate. 4 is a rectangular waveguide for introducing microwaves. Reference numeral 9 denotes a plasma extraction window for guiding the plasma generated in the plasma generation chamber 1 to the fitting 11 placed on the fitting 10. Reference numeral 13 denotes a magnetic coil for generating a magnetic field strength that satisfies the electron cyclo-l-ron mutual duck condition in a suitable region inside the plasma generation chamber 1;
It is also used to form a divergence 611 field for forming the plasma flow 8. A microwave source (not shown) is configured using, for example, a magnetron with a frequency of 2.45 GHz. Reference numeral 5 designates a cooling channel for the plasma generation chamber, and 6 and 7 designate a first gas introduction system and a second gas introduction system for gas regulators, which are used singly or in combination depending on the processing purpose.

例えは、窒化シリコン膜の形成には第1ガス導入系6よ
りガスを導入し、第2ガス導入系7から5it14ガス
を導入する。エツチングの場合は第1ガス導人千6また
は第2カス導入系7からcf!、2SF6.02なとの
エツチング用ガスを導入する。
For example, to form a silicon nitride film, gas is introduced from the first gas introduction system 6 and 5it14 gas is introduced from the second gas introduction system 7. In the case of etching, cf! from the first gas guide 16 or the second waste introduction system 7! , 2SF6.02 etching gas is introduced.

このような、薄膜形成やエツチングでの処理加工の試料
面内分布は、プラズマ生成簿≦1て1成されるプラズマ
密度、引出されるプラズマ流の密度などに依存しである
程度の不拘−性苓持っているため、大面積の試料に適用
するにζJ、さらに均性を向上させる必要がある。薄膜
の形成やエツチングの反応は、主に発散磁界の磁力線に
沿ってザイクロ)・ロン運動した電子と、電子とガス分
子との衝突により発生したイオンにより促進されること
から、発散磁界分布を制御することでプラズマ処理速度
の試着面内分布を改善することが考えられる。
The in-plane distribution of the sample during processing such as thin film formation or etching depends on the plasma density formed by the plasma generation table ≦ 1, the density of the drawn plasma flow, etc. Because it has ζJ, it is necessary to further improve the homogeneity when applying it to large-area samples. Thin film formation and etching reactions are mainly promoted by electrons that move along the magnetic field lines of the divergent magnetic field and by ions generated by collisions between electrons and gas molecules, so the divergent magnetic field distribution can be controlled. By doing so, it is possible to improve the distribution of plasma processing speed within the fitting surface.

第8図に、従来の磁界分布補正用コイルを付加したプラ
ズマ処理装置の概略構成図を示す。この図は試!4室を
拡大して示しており、他のNS分の構成は第7図と同様
である。試着台1oの裏側にソレノイドコイル14を配
置し、発散磁界用の磁気コイル13に対して逆方向電流
を流すことにより、試料面内の発散磁界分布を制御する
ものである。
FIG. 8 shows a schematic configuration diagram of a plasma processing apparatus to which a conventional magnetic field distribution correction coil is added. Try this diagram! The four chambers are shown in an enlarged view, and the configuration of the other NS portions is the same as in FIG. 7. A solenoid coil 14 is disposed on the back side of the fitting table 1o, and a reverse current is passed through the magnetic coil 13 for the divergent magnetic field to control the divergent magnetic field distribution within the sample plane.

[発明が解決し、ようとする課題] 第8図の構成により均一性を改善することはある程度可
能であるが、コイルがソレノイド状であるため、発散磁
界分布の制御が部分的になり、平坦な処理速度分布が得
られにくいこと、コイルの容積が大きくなるため試料台
とは別に設置場所を確保する必要があること、しかもコ
イルからの吸Mifス、ゴミの発生を防止するため、コ
イルを試料室の外に設置することなど、装置構成上いろ
いろ制限される問題が生じる。試料面内の磁界分布を最
適な分布に広範囲に制御でき、しかも小型で薄いコイル
かできれば、さらに処理面積の拡大、処理速度の向上な
ど大幅な特性向上が期待できるとともに装置構成が容易
になる。
[Problems to be solved and attempted by the invention] Although it is possible to improve the uniformity to some extent with the configuration shown in Fig. 8, since the coil is solenoid-shaped, the control of the divergent magnetic field distribution is only partial, resulting in flatness. It is difficult to obtain a uniform processing speed distribution, the volume of the coil is large, so it is necessary to secure an installation location separate from the sample stage, and in order to prevent the generation of Mifs and dust from the coil, it is difficult to install the coil. There are various problems with the device configuration, such as installation outside the sample chamber. If the magnetic field distribution in the sample plane can be controlled over a wide range to an optimal distribution, and if a small and thin coil can be created, significant improvements in characteristics such as an expansion of the processing area and an increase in processing speed can be expected, as well as ease of equipment configuration.

本発明は干述した従来の欠点を解決し、プラズマ流の発
散磁界分布を広範囲に制御し、処理速度の均一性を向上
させ、処理面積や処理速度を向上させつるプラズマ処理
装置を提伏することを目的とする。
The present invention solves the above-mentioned conventional drawbacks, and provides a plasma processing apparatus that can control the divergent magnetic field distribution of plasma flow over a wide range, improve the uniformity of processing speed, and improve the processing area and processing speed. The purpose is to

[課題を解決するための手段] 本発明はマイクロ波を利用してプラズマを生成し、プラ
ズマまたはプラズマ中の主としてイオンを試料に照射し
て処理を行うプラズマ処理装置において、試料を保持す
るための試着台の試料保持面と反対側の面に、試料台表
面近傍の磁界分布を制御するための少なくとも1個の偏
平コイルを具えたことを特徴とする。
[Means for Solving the Problems] The present invention provides a plasma processing apparatus that generates plasma using microwaves and processes the sample by irradiating the sample with plasma or mainly ions in the plasma. It is characterized in that at least one flat coil for controlling the magnetic field distribution in the vicinity of the sample stand surface is provided on the opposite side of the sample holding surface of the fitting stand.

[作 用] 本発明の偏平コイルは直径方向に渦巻き状に巻いた薄い
円板状のコイルであり、プラズマ生成室から引き出され
る発散磁界の試料台表面近傍の磁界分布を、コイルの巻
線密度分布、試着台とコイルとの距削、およびコイル電
流を設定することにより広範囲に制御し、均一性のよい
平坦なプラズマ処理速度を可能にする。コイルと試料台
との組合わせはコイル全体の厚さが薄いため、試料台と
体に構成することが可能であり、また、試着を冷却する
ために、冷却水な試才4台に循環する構造VずJlは、
コイルの冷却との併用もでき有効である。さらに、試料
台に試料を保持するだめの静電吸S方式および試料にバ
イアスを付加するRF印加ノJ式を採用し・た場合も、
試着台に本発明の偏平コイルを組込むことか可能である
[Function] The flat coil of the present invention is a thin disk-shaped coil spirally wound in the diametrical direction, and the magnetic field distribution near the sample stage surface of the divergent magnetic field extracted from the plasma generation chamber is determined by the winding density of the coil. By setting the distribution, the distance between the fitting table and the coil, and the coil current, it is possible to control over a wide range and achieve a flat plasma processing rate with good uniformity. The combination of the coil and sample stand is possible because the overall thickness of the coil is thin, so it is possible to configure the sample stand and the body, and in order to cool the sample, cooling water can be circulated to the four sample samples. The structure VzuJl is
It can also be used in conjunction with coil cooling and is effective. Furthermore, even when adopting the electrostatic absorption S method for holding the sample on the sample stage and the RF application J method for applying bias to the sample,
It is possible to incorporate the flat coil of the present invention into a fitting table.

[実施例] 以下に図面を参照して本発明の詳細な説明する。[Example] The present invention will be described in detail below with reference to the drawings.

第1図に本発明を実施したプラズマ処理装置の構成を示
す。第1図は試料室を拡大して示しており、他の部分の
構成は、第7図と同様である。プラズマ生成室1のプラ
ズマ引出し窓9を通って導か、iまたプラズマ流8によ
り、試料台10上の試料11をプラズマ処理する。その
試料台10の裏面に偏平コイル15を発散磁界発生用の
磁気コイル13と中心軸を一致させて配置した。偏平コ
イルは中心軸部から直径方向に渦巻状に巻いた構造で、
実験例ではコイル線として線径1.5mmのポリイミド
被覆銅線を用い、磁界強度を増すため、2枚重ねにして
あり、コイル全体の厚さは約:1mm 、直径はlO〜
70cm程度である。
FIG. 1 shows the configuration of a plasma processing apparatus in which the present invention is implemented. FIG. 1 shows an enlarged view of the sample chamber, and the configuration of other parts is the same as that in FIG. 7. A sample 11 on a sample stage 10 is subjected to plasma treatment by a plasma flow 8 introduced through a plasma extraction window 9 of the plasma generation chamber 1 . A flat coil 15 was placed on the back surface of the sample stage 10 so that its central axis coincided with that of the magnetic coil 13 for generating a divergent magnetic field. The flat coil has a structure in which it is spirally wound in the diametrical direction from the central axis.
In the experimental example, a polyimide-coated copper wire with a wire diameter of 1.5 mm was used as the coil wire, and in order to increase the magnetic field strength, it was stacked in two layers, and the overall thickness of the coil was approximately 1 mm, and the diameter was lO~
It is about 70cm.

このような構成によって、発11シ磁界で引出されたプ
ラズマ流の試料面内の磁界分布を、発散磁界と逆方向の
磁界を発生さセる偏平コイルにより制御する。発散磁界
のみの試才4面内の磁界強度は中央部か高< (115
G)円周部になるほどゆるやかに低下した(中心より9
cm 1lIffれた位置で100G)分布を持ってい
る。
With this configuration, the magnetic field distribution within the sample plane of the plasma flow drawn by the emitted magnetic field is controlled by the flat coil that generates a magnetic field in the opposite direction to the emitted magnetic field. The magnetic field strength in the four planes of the test case with only the divergent magnetic field is at the center or high < (115
G) It gradually decreased toward the circumference (9 from the center)
It has a distribution of 100G at the position of cm 1lIff.

本発明の偏平コイルを用いた効果を確認するため、酸化
シリコン膜について膜形成実験を行なった。膜形成条件
はこの実験では、02:30cc/m1nSit14:
30cc/+nj口、マイクロ波パワー  200Wと
した。試料は5インヂないし6インヂのS】ウェーハを
使用した。
In order to confirm the effect of using the flat coil of the present invention, a film formation experiment was conducted using a silicon oxide film. In this experiment, the film formation conditions were 02:30cc/m1nSit14:
30cc/+nj port, microwave power 200W. A 5-inch to 6-inch S] wafer was used as the sample.

第2図に円板状の偏平コイルの概略構成図を示す。コイ
ルは中心軸から直径方向へ渦巻状に順次巻いた巻線密度
の高いもので直径14cmであり、コイルと試料は5m
mmfした。第3図にこの円板状の偏平コイルを用いた
場合の磁界分布と膜形成速度分布を示す。このコイルの
&H磁界分布、コイル中央が最も磁界が強いピラミッド
状である。得られた膜形成速度分布はコイルを使用しな
い場合に比べて、コイル電流5八で中心部4cmの範囲
が平坦になり、さらにコイル電流7.5八では、中心部
7cmの範囲が平坦になった。
FIG. 2 shows a schematic configuration diagram of a disk-shaped flat coil. The coil has a diameter of 14 cm and has a high winding density that is spirally wound sequentially from the central axis in the diametrical direction, and the coil and sample are 5 m long.
mmf. FIG. 3 shows the magnetic field distribution and film formation rate distribution when this disc-shaped flat coil is used. The &H magnetic field distribution of this coil has a pyramid shape where the magnetic field is strongest at the center of the coil. The film formation rate distribution obtained is that when the coil current is 5.5 cm, the center 4 cm range is flat, and when the coil current is 7.5 cm, the center 7 cm range is flat, compared to when no coil is used. Ta.

第4図に、ドーナツ状の偏平コイルの概略構成図を示す
。コイル形状は、直径18cmで中心部の直径10cm
を中空にしたものて、このコイルと試料台との距離は多
少なだらかな磁界分布とするため10a+mとした。第
5図にこのドーナツ状の偏平コイルを用いた場合のその
磁界分布と膜形成速度分布を示す。このコイルの磁界分
布は、はぼ台形状となっており、この台形の上辺に相当
した部分がコイルの中空径10cmに対応したかたちと
なっている。実際の試料面内分布は発散磁界分布との合
成になり、直径10cmの外周部分が高い磁界強度とな
る。このコイルを使用した結果、膜形成速度分布は広範
囲にわたって、均一性の改善が認められ、たとえば試料
面の中心と±6.5cmの位置とではコイルを使用しな
いと±10%の不均一性かあるのに対し、コイル電流1
0Aでは±5%と、従来の半分に不均一性を低減できた
。第6図は、巻線密度を考えた場合の偏平コイルの概略
構成図を示す。コイル中央部はある程度間隔をとって巻
き、周辺部はつめて巻いた構造で、このコイルの磁界分
布はコイル中央部から円周部にゆるやかに低下した曲線
状をとるため、発散磁界の制御性か一段と高まり、さら
に試料面内分布の均一性の向上が図ねる。
FIG. 4 shows a schematic configuration diagram of a doughnut-shaped flat coil. The coil shape is 18cm in diameter with a center diameter of 10cm.
The coil was hollow, and the distance between this coil and the sample stage was set to 10 a+m in order to obtain a somewhat gentle magnetic field distribution. FIG. 5 shows the magnetic field distribution and film formation rate distribution when this doughnut-shaped flat coil is used. The magnetic field distribution of this coil has a trapezoidal shape, and the portion corresponding to the upper side of this trapezoid corresponds to the hollow diameter of the coil of 10 cm. The actual in-plane distribution of the sample is a combination of the diverging magnetic field distribution, and the outer peripheral portion with a diameter of 10 cm has a high magnetic field strength. As a result of using this coil, it was observed that the uniformity of the film formation rate distribution was improved over a wide range. For example, at a position ±6.5 cm from the center of the sample surface, the non-uniformity would be ±10% if the coil was not used. Whereas, the coil current 1
At 0 A, the nonuniformity was reduced to ±5%, which is half of the conventional level. FIG. 6 shows a schematic configuration diagram of a flat coil when winding density is considered. The coil has a structure in which the central part of the coil is wound with a certain interval, and the peripheral part is wound tightly.The magnetic field distribution of this coil takes a curved shape that gradually decreases from the central part of the coil to the circumference, making it easy to control the divergent magnetic field. In addition, the uniformity of the distribution within the sample plane can be further improved.

なお、本発明の変形として、磁界分布を設定した板状永
久磁石の利用や、本発明と軟鉄などの高透磁率旧料との
組合せによって、同様の効果をもたらす磁界分布を形成
することもできる。また、複数個の偏平コイルを組合わ
せて、磁界分布の制御性をさらに高めることも可能であ
る。
As a modification of the present invention, it is also possible to form a magnetic field distribution that provides the same effect by using a plate-shaped permanent magnet with a set magnetic field distribution, or by combining the present invention with a high magnetic permeability old material such as soft iron. . It is also possible to further improve the controllability of the magnetic field distribution by combining a plurality of flat coils.

[発明の効果コ 以上の説明から明らかなように、本発明の装置において
は偏平コイルを用い゛CC発磁磁界分イr]を広範囲に
制御できるようにしたので、プラズマ処理速度の均一性
が向上し、プラズマ処理面積の拡大、スルーブツトの向
上を実現できるとともに、装置構成上は、試料台との組
合わせが容易になる利点がある。
[Effects of the Invention] As is clear from the above explanation, in the apparatus of the present invention, the flat coil is used to control the CC magnetic field component over a wide range, which improves the uniformity of the plasma processing speed. This has the advantage that it is possible to expand the plasma processing area, improve throughput, and in terms of the device configuration, it can be easily combined with a sample stage.

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

第1図は本発明の実施例の概要図、 第2図は円板状偏平コイルの概略断面図、第3図は円板
状偏平コイルを用いた場合の磁界分布と5in2膜形成
膜形分速を示す図、第4図はドーナツ状偏平コイルの概
略断面図、 第5図はドーナツ状偏平コイルを用いた場合の磁界分布
とSiO□膜形成速度分布を示す図、第6図は巻線密度
を変えた偏平コイルの概略断面図、 第7図はプラズマ処理装置の基本構成図、第8図は従来
の磁界分布補正用コイルを用いた装置の概要図である。 1・・・プラズマ生成室、 2・・・試料室、 3・・・マイクロ波導入窓、 4・・・矩形導波管、 5・・・冷却水路、 6・・・第1ガス導入系、 7・・・第2ガス導人系、 8・・・プラズマ流、 9・・・プラズマ引出し窓、 10・・・試料台、 11・・・試料、 12・・・排気系、 13・・・磁気コイル、 1イ・・・ソレノイドコイル、 15・・・偏平コイル。
Fig. 1 is a schematic diagram of an embodiment of the present invention, Fig. 2 is a schematic cross-sectional view of a disc-shaped flat coil, and Fig. 3 is a diagram showing magnetic field distribution and 5in2 film formation film shape when using a disc-shaped flat coil. Figure 4 is a schematic cross-sectional view of a donut-shaped flat coil, Figure 5 is a diagram showing the magnetic field distribution and SiO□ film formation rate distribution when a donut-shaped flat coil is used, and Figure 6 is a diagram showing the winding speed. FIG. 7 is a schematic cross-sectional view of flat coils with different densities, FIG. 7 is a basic configuration diagram of a plasma processing apparatus, and FIG. 8 is a schematic diagram of an apparatus using a conventional magnetic field distribution correction coil. DESCRIPTION OF SYMBOLS 1... Plasma generation chamber, 2... Sample chamber, 3... Microwave introduction window, 4... Rectangular waveguide, 5... Cooling channel, 6... First gas introduction system, 7... Second gas guide system, 8... Plasma flow, 9... Plasma extraction window, 10... Sample stage, 11... Sample, 12... Exhaust system, 13... Magnetic coil, 1. Solenoid coil, 15. Flat coil.

Claims (1)

【特許請求の範囲】[Claims] 1)マイクロ波を利用してプラズマを生成し、該プラズ
マまたは該プラズマ中の主としてイオンを試料に照射し
て処理を行うプラズマ処理装置において、前記試料を保
持するための試料台の試料保持面と反対側の面に、試料
台表面近傍の磁界分布を制御するための少なくとも1個
の偏平コイルを具えたことを特徴とするプラズマ処理装
置。
1) In a plasma processing apparatus that generates plasma using microwaves and processes a sample by irradiating the plasma or mainly ions in the plasma, a sample holding surface of a sample stage for holding the sample; A plasma processing apparatus characterized in that the opposite surface is provided with at least one flat coil for controlling the magnetic field distribution near the surface of the sample stage.
JP7394189A 1989-03-28 1989-03-28 Plasma processing device Expired - Lifetime JPH064917B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7394189A JPH064917B2 (en) 1989-03-28 1989-03-28 Plasma processing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7394189A JPH064917B2 (en) 1989-03-28 1989-03-28 Plasma processing device

Publications (2)

Publication Number Publication Date
JPH02254170A true JPH02254170A (en) 1990-10-12
JPH064917B2 JPH064917B2 (en) 1994-01-19

Family

ID=13532639

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7394189A Expired - Lifetime JPH064917B2 (en) 1989-03-28 1989-03-28 Plasma processing device

Country Status (1)

Country Link
JP (1) JPH064917B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04235283A (en) * 1990-12-31 1992-08-24 Semiconductor Energy Lab Co Ltd Apparatus and method for forming coating film

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04235283A (en) * 1990-12-31 1992-08-24 Semiconductor Energy Lab Co Ltd Apparatus and method for forming coating film

Also Published As

Publication number Publication date
JPH064917B2 (en) 1994-01-19

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