JPH0480384A - Plasma etching device - Google Patents

Plasma etching device

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Publication number
JPH0480384A
JPH0480384A JP19206090A JP19206090A JPH0480384A JP H0480384 A JPH0480384 A JP H0480384A JP 19206090 A JP19206090 A JP 19206090A JP 19206090 A JP19206090 A JP 19206090A JP H0480384 A JPH0480384 A JP H0480384A
Authority
JP
Japan
Prior art keywords
electromagnet
plasma
etching
counter electrode
magnetic poles
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
JP19206090A
Other languages
Japanese (ja)
Other versions
JP2969528B2 (en
Inventor
Hideki Fujimoto
秀樹 藤本
Toshio Hayashi
俊雄 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.)
Ulvac Inc
Original Assignee
Ulvac Inc
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 Ulvac Inc filed Critical Ulvac Inc
Priority to JP19206090A priority Critical patent/JP2969528B2/en
Publication of JPH0480384A publication Critical patent/JPH0480384A/en
Application granted granted Critical
Publication of JP2969528B2 publication Critical patent/JP2969528B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Drying Of Semiconductors (AREA)

Abstract

PURPOSE:To uniformalize etching and also to prevent etching defective by annularly arranging the respective magnet poles of a multipolar electromagnet having even pieces of magnetic poles in the prescribed intervals to the external periphery of the cylindrical side wall of an etching chamber and regulating the adjacent magnetic poles to reverse polarities with each other in a plasma etching device. CONSTITUTION:The respective magnetic poles of a multipolar electromagnet 14 having even pieces of magnetic poles 13 are annularly arranged in the prescribed intervals to the external periphery of the cylindrical side wall 1 of an etching chamber 2. The adjacent magnetic poles 13 are regulated to the reverse polarities 13. Plasma is generated by discharge caused between a counter electrode 5 and a base plate electrode 8. This plasma receives the effect of the magnetic field of a double annular electromagnet 6 and is made to high density in the vicinity of the counter electrode 5 and etches a base plate 7 at high velocity. The plasma is contained into the space between the counter electrode 5 and the base plate electrode 8 by a cusp field formed by the multipolar electromagnet 14 arranged to the external periphery of the cylindrical side wall 1 of the etching chamber 2. Dissociation of gas in this space is advanced and homogenizing of plasma in the space is caused and uniformity of etching is enhanced.

Description

【発明の詳細な説明】 (産業上の利用分野) この発明はエツチング室の円筒形の側壁の外周に偶数個
の磁極をもった多極電磁石を配置したプラズマエツチン
グ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 plasma etching apparatus in which a multipolar electromagnet having an even number of magnetic poles is arranged around the outer periphery of a cylindrical side wall of an etching chamber.

(従来の技術) 従来のプラズマエツチング装置は第6図に示されており
、同図において、円筒形の側壁1をもったエツチング室
2の上部は上面板3で覆われ、その上面板3の下部はガ
ス噴出口4と兼用になったアース電位の平板な対向電極
5が設けられ、また、上面板3の上部は二重環状電磁石
6が設けられ、平板な対向電極5の背後に二重環状電磁
石6が位置するようになっている。二重環状電磁石6は
中央ヨーク6aの回りに直径の異なる2つの環状ヨーク
6b、6cが同芯状に配列され、そして、中央ヨーク6
aと環状ヨーク6bとの間、および環状ヨーク6bと環
状ヨーク6cとの間にそれぞれコイル6d、6eが設け
られた構造になっている。
(Prior Art) A conventional plasma etching apparatus is shown in FIG. 6, in which the upper part of an etching chamber 2 having a cylindrical side wall 1 is covered with a top plate 3. A flat counter electrode 5 at ground potential that also serves as the gas outlet 4 is provided at the bottom, and a double annular electromagnet 6 is provided at the top of the top plate 3. An annular electromagnet 6 is located there. The double annular electromagnet 6 has two annular yokes 6b and 6c having different diameters arranged concentrically around a central yoke 6a.
It has a structure in which coils 6d and 6e are provided between the annular yoke 6a and the annular yoke 6b, and between the annular yoke 6b and the annular yoke 6c, respectively.

エツチング室2の下方には基板7を載置した平板な基板
電極8が位置し、その基板電極8はエツチング室2内に
おいて平板な対向電極5と距離をおいて対向している。
A flat substrate electrode 8 on which a substrate 7 is placed is located below the etching chamber 2, and the substrate electrode 8 faces a flat counter electrode 5 at a distance within the etching chamber 2.

ガスはガス導入部9より対向電極5内に流れ込み、そし
て、対向電極5のガス噴出口4より基板電極8方向に噴
出するようになっている。なお、図において、lOは基
板電極8を冷却する冷却部、11は基板電極8に13.
5′6 M Hzの高周波電力を印加する高周波電源で
ある。
The gas flows into the counter electrode 5 from the gas introduction part 9, and is ejected from the gas outlet 4 of the counter electrode 5 in the direction of the substrate electrode 8. In the figure, lO is a cooling unit that cools the substrate electrode 8, and 11 is a cooling unit 13 for cooling the substrate electrode 8.
This is a high frequency power source that applies high frequency power of 5'6 MHz.

このようなプラズマエツチング装置においては、対向電
極5と基板電極8との間で放電が起こり、プラズマが発
生するようになるが、そのプラズマは二重環状電磁石6
の磁場の影響を受けて、対向電極5の近傍で高密度にな
っている。そして、この高密度になっているプラズマ中
のイオンか基板電極8に引き寄せられ、基板電極8上の
基板7と衝突して、基板7を高速度でエツチングするよ
うになる。
In such a plasma etching apparatus, a discharge occurs between the counter electrode 5 and the substrate electrode 8, and plasma is generated.
Under the influence of the magnetic field, the density is high near the counter electrode 5. Ions in this high-density plasma are then attracted to the substrate electrode 8 and collide with the substrate 7 on the substrate electrode 8, etching the substrate 7 at a high speed.

(発明が解決しようとする課題) 従来のプラズマエツチング装置は、上記のように二重環
状電磁石6の磁場の影響を受けて発生した高密度なプラ
ズマ中のイオンが基板を高速度でエツチングするように
なるが、二重環状電磁石6の磁場は均一ではなく、不均
一であるため、エツチングも均一にならない問題が起き
た。そのため、対向電極5と基板電極8との間隔を狭め
ることができなくなり、その結果、エツチング速度が制
限されたり、あるいは電極の間隔が広くなって、基板7
に対するイオン衝撃が大きくなり、集積回路の基板の電
気特性を悪くする等の問題を引き起こした。更に、二重
環状電磁石6の磁場の影響を受けながらプラズマを発生
させるときには、圧力が1O−3Torr台で行われる
ため、プラズマが対向電極5や基板電極8の外にも広が
り、その結果、エツチングの効率が落ちたり、あるいは
対向電極5や基板電極8の外側で再重合による堆積を引
き起こし、それが基板に付着してマスクとなり、エツチ
ング残りを起こす問題が起きた。更にそのうえ、対向電
極5や基板電極8の外に広がったプラズマによりエツチ
ング室2の円筒形の側壁lがスパッタされ、その粒子が
基板7に不純物として混入してしまう等の問題も起きた
(Problems to be Solved by the Invention) The conventional plasma etching apparatus is designed so that the ions in the high-density plasma generated under the influence of the magnetic field of the double ring electromagnet 6 as described above etch the substrate at high speed. However, since the magnetic field of the double ring electromagnet 6 is not uniform but non-uniform, a problem arose in that the etching was not uniform. Therefore, the distance between the counter electrode 5 and the substrate electrode 8 cannot be narrowed, and as a result, the etching rate is limited, or the distance between the electrodes becomes wide, and the substrate 7
The ion bombardment on the substrate increased, causing problems such as deterioration of the electrical characteristics of the integrated circuit substrate. Furthermore, when plasma is generated under the influence of the magnetic field of the double ring electromagnet 6, the pressure is on the order of 10-3 Torr, so the plasma spreads outside the counter electrode 5 and the substrate electrode 8, resulting in etching. This has resulted in problems such as a decrease in the efficiency of etching, or deposition due to repolymerization on the outside of the counter electrode 5 and substrate electrode 8, which adheres to the substrate and forms a mask, resulting in etching residue. Furthermore, problems such as sputtering of the cylindrical side wall 1 of the etching chamber 2 by the plasma spreading outside the counter electrode 5 and the substrate electrode 8 have occurred, and the particles thereof are mixed into the substrate 7 as impurities.

この発明の目的は、従来の問題を解決して、エツチング
を均一にするとともに、イオン衝撃をなくし、堆積によ
る汚染や周囲の側壁からの汚染をエツチング不良のない
高速エツチングを可能にするプラズマエツチング装置を
提供することにある。
The purpose of this invention is to provide a plasma etching apparatus that solves the conventional problems, makes etching uniform, eliminates ion bombardment, and enables high-speed etching without etching defects due to contamination due to deposition or contamination from surrounding sidewalls. Our goal is to provide the following.

(課題を解決するための手段) 上記目的を達成するために、この発明は、上記のような
プラズマエツチング装置において、エツチング室の円筒
形の側壁の外周に、偶数個の磁極をもった多極電磁石の
各磁極を所定の間隔で環状に配置し、隣接する磁極を相
互に逆極性にして、放電を多極電磁石によって封じ込む
と共に、多極電磁石によって形成される多極磁場を制御
可能にしたことを特徴とするものである。
(Means for Solving the Problems) In order to achieve the above object, the present invention provides a plasma etching apparatus as described above, in which a multi-pole etching device having an even number of magnetic poles is provided on the outer periphery of the cylindrical side wall of the etching chamber. Each magnetic pole of the electromagnet is arranged in a ring shape at a predetermined interval, and adjacent magnetic poles are made to have opposite polarity to each other, allowing the multipolar electromagnet to confine discharge and control the multipolar magnetic field formed by the multipolar electromagnet. It is characterized by this.

(作用) この発明のプラズマエツチング装置においては、エツチ
ング室の円筒形の側壁の外周に、偶数個の磁極をもった
多極電磁石の各磁極を所定の間隔で環状に配置し、隣接
する磁極を相互に逆極性にしているので、カスプ磁場が
形成されるようになる。
(Function) In the plasma etching apparatus of the present invention, the magnetic poles of a multipolar electromagnet having an even number of magnetic poles are arranged in a ring shape at predetermined intervals around the outer periphery of the cylindrical side wall of the etching chamber, and adjacent magnetic poles are arranged in a ring shape at predetermined intervals. Since the polarities are opposite to each other, a cusp magnetic field is formed.

したがって、対向電極と基板電極との間の放電によって
発生したプラズマはカスプ磁場の影響を受け、プラズマ
が周囲に広がるのが抑えられ、プラズマが対向電極と基
板電極との間に集中するようになる。そのため、エツチ
ングの効率が向上し、均一なエツチングが可能になると
ともに、周囲での堆積やスパッタがなくなり、基板への
不純物の混入が抑制されるようになった。更に、多極電
磁石によって形成される多極磁場を制御することによっ
て、カスブ磁場の強度を変えて、放電が集中する領域を
変えることが可能になり、基板に応じた放電領域を得る
ことが可能になった。
Therefore, the plasma generated by the discharge between the counter electrode and the substrate electrode is affected by the cusp magnetic field, suppressing the plasma from spreading to the surroundings, and causing the plasma to concentrate between the counter electrode and the substrate electrode. . As a result, etching efficiency has been improved, uniform etching has become possible, and deposition and sputtering around the substrate has been eliminated, and contamination of impurities into the substrate has been suppressed. Furthermore, by controlling the multipolar magnetic field formed by the multipolar electromagnet, it is possible to change the strength of the cusp magnetic field and change the area where the discharge is concentrated, making it possible to obtain a discharge area that matches the substrate. Became.

(実施例) 以下、この発明の実施例について図面を参照しながら説
明する。
(Example) Hereinafter, an example of the present invention will be described with reference to the drawings.

第1図はこの発明の実施例を示しており、同図において
、従来の装置を示す第5図と同符号のものは同一につき
その説明を省略するが、この発明の実施例は従来の装置
を改良して、工、ツチング室2の円筒形の側壁lの外周
に、偶数個の磁極13をもった多極電磁石14の各磁極
を所定の間隔で環状に配置し、隣接する磁極13を相互
に逆極性にしたものである。磁極13は第2図および第
3図に示すようにヨーク15の一部分を内側に当間隔に
張り出して形成した張り出し部15aの回りにコイル1
6を巻いて作られたものである。磁極13の極性を逆極
性にする場合には、隣合ったコイルの巻き方を逆にする
か、またはコイルへの印加電流を逆向きにするかしてな
される。
FIG. 1 shows an embodiment of the present invention. In the same figure, the same reference numerals as in FIG. By improving the technique, each magnetic pole of a multipolar electromagnet 14 having an even number of magnetic poles 13 is arranged in a ring shape at a predetermined interval on the outer periphery of the cylindrical side wall l of the cutting chamber 2, and adjacent magnetic poles 13 are arranged in a ring shape. They have mutually opposite polarities. As shown in FIGS. 2 and 3, the magnetic pole 13 is formed by extending a portion of the yoke 15 inward at equal intervals.
It is made by winding 6. When the polarity of the magnetic pole 13 is reversed, it is done by reversing the winding of adjacent coils or by reversing the direction of the current applied to the coils.

このような実施例においては、従来と同様に、対向電極
5と基板電極8との間の放電によりプラズマが発生する
ようになるが、そのプラズマは二重環状電磁石6の磁場
の影響を受けて、対向電極5の近傍で高密度になり、基
板7を高速度でエツチングすることが可能になる。だが
、実施例では従来と異なり、エツチング室2の円筒形の
側壁1の外周に配置した多極電磁石14によって形成さ
れたカスブ磁場により、プラズマが対向電極5と基板電
極8との間の空間に封じ込められ、その空間でのガスの
解離が進み、その空間内でのプラズマの均質化が起こり
、エツチングの均一性が向上するようになる。また、カ
スブ磁場の影響により、プラズマが対向電極5と基板電
極8との間の空間の外に広がるのが抑えられるため、エ
ツチング室2の円筒形の側壁lをスパッタしたり、ある
いは堆積がなくな轢、基板7への不純物の混入が抑制さ
れるようになる。更に、多極電磁石14の各磁極13の
コイル16に流す電流値を制御することによって、カス
ブ磁場の強度を制御することかでき、そのため、放電が
集中する領域を変えることが可能になり、基板に応じた
放電領域を得ることが可能になった。
In such an embodiment, plasma is generated by the discharge between the counter electrode 5 and the substrate electrode 8, as in the conventional case, but the plasma is influenced by the magnetic field of the double ring electromagnet 6. , the etching density becomes high near the counter electrode 5, making it possible to etch the substrate 7 at a high speed. However, in this embodiment, unlike the conventional etching chamber 2, plasma is caused to flow into the space between the counter electrode 5 and the substrate electrode 8 due to the cusp magnetic field formed by the multipolar electromagnet 14 disposed around the outer periphery of the cylindrical side wall 1 of the etching chamber 2. The gas is confined, gas dissociation progresses in that space, the plasma becomes homogenized in that space, and the uniformity of etching improves. In addition, because the plasma is prevented from spreading outside the space between the counter electrode 5 and the substrate electrode 8 due to the influence of the cusp magnetic field, there is no sputtering or deposition on the cylindrical side wall l of the etching chamber 2. This also suppresses impurities from entering the substrate 7. Furthermore, by controlling the current value flowing through the coil 16 of each magnetic pole 13 of the multipole electromagnet 14, it is possible to control the strength of the cusp magnetic field. It became possible to obtain a discharge area according to the

ところで、上記実施例は基板電極8に1356MHzの
高周波電力を印加し、対向電極5をアース電位にしてい
るが、これを反対にして、基板電極8をアース電位にし
、対向電極5に1356MHzの高周波電力を印加して
もよい。また、第4図に示すように対向電極5とエツチ
ング室2の円筒形の側壁1とを絶縁物I7で絶縁し、そ
の一方をアース電位とし、他方に13.56MHzの高
周波電力を印加し、かつ基板電極8に100KHz 〜
600 KHzもしくは13.56MHzの高周波電力
を印加してもよい。更に、多極電磁石の構造を第5図に
示すようなものを使用してもよい。
By the way, in the above embodiment, a high frequency power of 1356 MHz is applied to the substrate electrode 8 and the counter electrode 5 is set to the ground potential. Electric power may also be applied. Further, as shown in FIG. 4, the counter electrode 5 and the cylindrical side wall 1 of the etching chamber 2 are insulated by an insulator I7, one of which is set at ground potential, and a high frequency power of 13.56 MHz is applied to the other. And 100KHz to substrate electrode 8
High frequency power of 600 KHz or 13.56 MHz may be applied. Furthermore, a multipole electromagnet structure as shown in FIG. 5 may be used.

(発明の効果) この発明は上記のようにエツチング室の円筒形の側壁の
外周に、偶数個の磁極をもった多極電磁石の各磁極を所
定の間隔で環状に配置し、隣接する磁極を相互に逆極性
にして、放電を多極電磁石によって封じ込むと共に、多
極電磁石によって形成される多極磁場を制御可能にして
いるから、次のような効果が奏される。
(Effects of the Invention) As described above, the present invention arranges the magnetic poles of a multipolar electromagnet having an even number of magnetic poles in a ring shape at predetermined intervals on the outer periphery of the cylindrical side wall of the etching chamber. Since the polarities are mutually opposite and the discharge is confined by the multipolar electromagnet, and the multipolar magnetic field formed by the multipolar electromagnet can be controlled, the following effects are achieved.

(1)多極電磁石によりカスブ磁場が形成され、プラズ
マが対向電極と基板電極との間の空間に封じ込められ、
その空間でのガスの解離が進み、その空間内でのプラズ
マの均質化が起こり、エツチングの均一性が向上するよ
うになる。
(1) A cusp magnetic field is formed by a multipole electromagnet, and plasma is confined in the space between the counter electrode and the substrate electrode,
Gas dissociation progresses in that space, plasma becomes homogenized within that space, and etching uniformity improves.

(2)カスブ磁場の影響により、プラズマが対向電極と
基板電極との間の空間の外に広がるのが抑えられるため
、エツチング室の円筒形の側壁をスパッタしたり、ある
いは堆積がなくなり、基板への不純物の混入が抑制され
るようになる。
(2) Due to the effect of the cusp magnetic field, the plasma is prevented from spreading outside the space between the counter electrode and the substrate electrode, so there is no sputtering or deposition on the cylindrical side wall of the etching chamber, and there is no deposition on the substrate. The contamination of impurities is suppressed.

(3)多極電磁石によって形成される多極磁場を制御す
ることによって、カスブ磁場の強度を変えて、放電が集
中する領域を変えることが可能になり、基板に応じた放
電領域を得ることが可能になる。
(3) By controlling the multipolar magnetic field formed by the multipolar electromagnet, it is possible to change the area where the discharge is concentrated by changing the strength of the cusp magnetic field, and it is possible to obtain a discharge area according to the substrate. It becomes possible.

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

第1図はこの発明の実施例を示す説明図、第2図は第1
図のI−I線で切断した断面図、第3図は第1図の多極
電磁石の磁極の一部を示す斜視図、第4図はこの発明の
その他の実施例を示す説明図、第5図はこの発明のその
他の実施例に用いられる多極電磁石の説明図である。第
6図は従来のプラズマエツチング装置を示す説明図であ
る。 図中、 l・・・・・エツチング室の円筒形の側壁2・・・・・
エツチング室 4・・・・・ガス噴出口 5・・・・・対向電極 6・・・・・二重環状電磁石 7・・・・・基板 8・・・・・基板電極 11・・・・高周波電源 13・・・・多極電磁石の磁極 14・・・・多極電磁石 15 ・ 5a l 6 ・ I 7 ・ ・ヨーク ・ヨークの張り出し部 ・コイル ・絶縁物
FIG. 1 is an explanatory diagram showing an embodiment of this invention, and FIG.
3 is a perspective view showing a part of the magnetic poles of the multipolar electromagnet shown in FIG. 1, FIG. 4 is an explanatory view showing another embodiment of the present invention, and FIG. FIG. 5 is an explanatory diagram of a multipolar electromagnet used in another embodiment of the present invention. FIG. 6 is an explanatory diagram showing a conventional plasma etching apparatus. In the figure, l... Cylindrical side wall 2 of the etching chamber...
Etching chamber 4... Gas outlet 5... Counter electrode 6... Double annular electromagnet 7... Substrate 8... Substrate electrode 11... High frequency Power supply 13... Magnetic pole of multipolar electromagnet 14... Multipolar electromagnet 15 ・ 5a l 6 ・ I 7 ・ ・Yoke, yoke overhang, coil, insulator

Claims (4)

【特許請求の範囲】[Claims] 1.背後に電磁石を設けた平板な対向電極と、同じく平
板な基板電極とを円筒形の側壁を持ったエッチング室内
において距離をおいて対向して配置し、平板な対向電極
のガス噴出口よりガスを平板な基板電極方向に噴出させ
、放電により発生するプラズマによって、基板電極上の
基板をエッチングするプラズマエッチング装置において
、上記エッチング室の円筒形の側壁の外周に、偶数個の
磁極をもった多極電磁石の各磁極を所定の間隔で環状に
配置し、隣接する磁極を相互に逆極性にして、上記放電
を多極電磁石によって封じ込むと共に、多極電磁石によ
って形成される多極磁場を制御可能にしたことを特徴と
するプラズマエッチング装置。
1. A flat counter electrode with an electromagnet behind it and a substrate electrode, which is also a flat plate, are placed facing each other at a distance in an etching chamber with a cylindrical side wall, and gas is injected from the gas outlet of the flat counter electrode. In a plasma etching apparatus that etches the substrate on the substrate electrode with plasma ejected in the direction of a flat substrate electrode and generated by discharge, a multipole having an even number of magnetic poles is installed on the outer periphery of the cylindrical side wall of the etching chamber. Each magnetic pole of the electromagnet is arranged in a ring shape at a predetermined interval, and adjacent magnetic poles are made to have opposite polarity to each other, so that the above discharge is contained by the multipolar electromagnet, and the multipolar magnetic field formed by the multipolar electromagnet can be controlled. A plasma etching device characterized by:
2.上記電磁石は二重環状電磁石であることを特徴とす
る請求項1記載のプラズマエッチング装置。
2. 2. The plasma etching apparatus according to claim 1, wherein said electromagnet is a double annular electromagnet.
3.上記対向電極および基板電極のいづれか一方に13
.56MHzの高周波電力を印加し、他方をアース電位
にしたことを特徴とする請求項1又は2記載のプラズマ
エッチング装置。
3. 13 on either one of the counter electrode and the substrate electrode.
.. 3. The plasma etching apparatus according to claim 1, wherein a high frequency power of 56 MHz is applied, and the other end is set at ground potential.
4.上記対向電極とエッチング室の円筒形の側壁とを絶
縁し、一方をアース電位とし、他方に13.56MHz
の高周波電力を印加し、かつ上記基板電極に100KH
z〜600KHzもしくは13.56MHzの高周波電
力を印加することを特徴とする請求項1又は2記載のプ
ラズマエッチング装置。
4. The above-mentioned counter electrode and the cylindrical side wall of the etching chamber are insulated, one of them is set to ground potential, and the other is set to 13.56 MHz.
high frequency power of 100 KH is applied to the above substrate electrode.
3. The plasma etching apparatus according to claim 1, wherein a high frequency power of 13.56 MHz or 13.56 MHz is applied.
JP19206090A 1990-07-20 1990-07-20 Plasma etching equipment Expired - Lifetime JP2969528B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19206090A JP2969528B2 (en) 1990-07-20 1990-07-20 Plasma etching equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19206090A JP2969528B2 (en) 1990-07-20 1990-07-20 Plasma etching equipment

Publications (2)

Publication Number Publication Date
JPH0480384A true JPH0480384A (en) 1992-03-13
JP2969528B2 JP2969528B2 (en) 1999-11-02

Family

ID=16284957

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19206090A Expired - Lifetime JP2969528B2 (en) 1990-07-20 1990-07-20 Plasma etching equipment

Country Status (1)

Country Link
JP (1) JP2969528B2 (en)

Also Published As

Publication number Publication date
JP2969528B2 (en) 1999-11-02

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