[go: up one dir, main page]

JP3357737B2 - Discharge plasma processing equipment - Google Patents

Discharge plasma processing equipment

Info

Publication number
JP3357737B2
JP3357737B2 JP01937494A JP1937494A JP3357737B2 JP 3357737 B2 JP3357737 B2 JP 3357737B2 JP 01937494 A JP01937494 A JP 01937494A JP 1937494 A JP1937494 A JP 1937494A JP 3357737 B2 JP3357737 B2 JP 3357737B2
Authority
JP
Japan
Prior art keywords
counter electrode
electrode
radius
frequency power
substrate
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
Application number
JP01937494A
Other languages
Japanese (ja)
Other versions
JPH07230987A (en
Inventor
俊雄 林
正文 田辺
秀夫 坪井
正博 伊藤
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 JP01937494A priority Critical patent/JP3357737B2/en
Publication of JPH07230987A publication Critical patent/JPH07230987A/en
Application granted granted Critical
Publication of JP3357737B2 publication Critical patent/JP3357737B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Plasma Technology (AREA)
  • Chemical Vapour Deposition (AREA)
  • Drying Of Semiconductors (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、プラズマを利用して、
半導体或いは電子部品、その他の基板に対してエッチン
グ、アッシング或いはプラズマCVD等の処理を行なう
放電プラズマ処理装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention
The present invention relates to a discharge plasma processing apparatus that performs processing such as etching, ashing, or plasma CVD on semiconductors, electronic components, and other substrates.

【0002】[0002]

【従来の技術】プラズマ生成に誘電体隔壁を通して高周
波電力を導入する、いわゆる、誘導結合放電方式は、従
来からエッチング、プラズマCVD等に用いられてき
た。添付図面の図3には誘導結合放電型のエッチング装
置の一例を示し、Aは真空チャンバーで、その内部には
基板Bを装着する基板電極Cが配置され、この基板電極
Cは高周波バイアス電源Dに接続されている。基板電極
Cに対向した位置には対向電極Eが誘電体隔壁Fを介し
て取付けられている。誘電体隔壁FのまわりにはRFコイ
ルGが設けられている。図3に示すような従来の誘導結
合放電型のエッチング装置では、基板が小さい場合に
は、処理速度の均一性はそれほど問題になっていなかっ
た。しかしながら、最近、8インチウエハが用いられる
ようになってきたため誘導結合方式における処理均一性
が問題となってきた。誘導結合方式によるエッチングで
は、誘導結合によって生成されるプラズマの基板方向へ
の拡散が利用され、プラズマ生成部と基板との距離が基
板と真空チャンバー側壁との距離よりも長いと、均一プ
ラズマを生成しても拡散過程でチャンバー側壁への拡散
によるプラズマの損失が多くなり、基板表面でのプラズ
マ均一性が得られない。これを避けるため、プラズマ生
成部を基板に近づけることが提案されてきたが、基板交
換のための搬送機構が複雑になり、装置の信頼性を低下
させる原因となるなどの別の問題が発生する。また、基
板電極に印加する高周波バイアス電力をプラズマ生成の
ための高周波電力よりも高くして均一性をよくすること
も提案されてきたが、この方法では誘導結合の利点を生
かしきれないことになる。
2. Description of the Related Art A so-called inductively coupled discharge system, in which high-frequency power is introduced through a dielectric partition for plasma generation, has conventionally been used for etching, plasma CVD and the like. FIG. 3 of the accompanying drawings shows an example of an inductively coupled discharge type etching apparatus. A is a vacuum chamber, in which a substrate electrode C for mounting a substrate B is arranged. It is connected to the. At a position facing the substrate electrode C, a counter electrode E is mounted via a dielectric partition F. An RF coil G is provided around the dielectric partition F. In the conventional inductively coupled discharge type etching apparatus as shown in FIG. 3, when the substrate is small, uniformity of the processing speed has not been a serious problem. However, recently, the use of 8-inch wafers has led to a problem of processing uniformity in the inductive coupling method. In the etching by the inductive coupling method, the diffusion of the plasma generated by the inductive coupling in the direction of the substrate is used. If the distance between the plasma generating unit and the substrate is longer than the distance between the substrate and the side wall of the vacuum chamber, uniform plasma is generated. Even in the diffusion process, plasma loss due to diffusion to the chamber side wall increases, and plasma uniformity on the substrate surface cannot be obtained. In order to avoid this, it has been proposed to move the plasma generation unit closer to the substrate. However, another problem arises that the transport mechanism for replacing the substrate becomes complicated and causes a reduction in the reliability of the apparatus. . It has also been proposed to improve the uniformity by increasing the high-frequency bias power applied to the substrate electrode higher than the high-frequency power for plasma generation, but this method cannot take advantage of the inductive coupling. .

【0003】[0003]

【発明が解決しようとする課題】誘導結合プラズマを利
用して大面積、高均一エッチングを達成するためには、
基板表面におけるプラズマの高い均一性が必要にある。
ところが、均一性の高いプラズマを形成しても拡散過程
で側壁へのプラズマ損失が多いため、基板表面上では均
一なプラズマ分布とはならない。これを均一にする方法
は種々提案されているが、誘導結合方式の利点を生かし
きっていないことや、基板搬送系が複雑になり、装置全
体の信頼性が低くなる等の問題があった。そこで、本発
明は、誘導結合プラズマを利用する従来の処理装置の問
題点を解決して、高均一処理を可能とした信頼性の高い
処理装置を提供することを目的としている。
In order to achieve a large area and high uniform etching using inductively coupled plasma,
High uniformity of the plasma on the substrate surface is required.
However, even if highly uniform plasma is formed, a large amount of plasma is lost to the side wall during the diffusion process, so that a uniform plasma distribution is not obtained on the substrate surface. Various methods have been proposed to make this uniform, but there have been problems such as not taking full advantage of the inductive coupling method, complicating the substrate transfer system, and lowering the reliability of the entire apparatus. Accordingly, an object of the present invention is to solve the problems of the conventional processing apparatus using inductively coupled plasma and to provide a highly reliable processing apparatus capable of performing highly uniform processing.

【0004】[0004]

【課題を解決するための手段】上記の目的を達成するた
めに、本発明によれば、誘電体隔壁を通して真空チャン
バー内に高周波電力を導入してプラズマを生成させるア
ンテナを備え、被処理物を処理するために高周波バイア
スを印加できる機構を備え、真空チャンバー内でプラズ
マを利用して被処理物を処理するようにした放電プラズ
マ処理装置において、被処理物の載置される高周波電力
印加電極と対向して設けた対向電極を高周波電力印加電
極に向って凸状に構成し、高周波電力印加電極と対向電
極との距離を、被処理物の半径と凸状に構成した対向電
極の半径との関係に基づいて設定したことを特徴として
いる。好ましくは、対向電極は高周波電力印加電極に向
かってのびた円柱状突起部かまたは断面半楕円形の突起
部を備えることができる。対向電極が円柱状突起部を備
えている場合には、突起部の先端と高周波電力印加電極
との距離を、被処理物の半径と突起部を備えた対向電極
の半径との差にほぼ等しくなるように構成され得、また
対向電極は高周波電力印加電極に向かってのびた円柱状
突起部かまたは断面半楕円形の突起部を備えている場合
には、突起部の先端と高周波電力印加電極との距離を、
被処理物の半径と突起部を備えた対向電極の基部の半径
の半分との差にほぼ等しくなるように構成され得る。
According to the present invention, there is provided, in accordance with the present invention, an antenna for generating plasma by introducing high-frequency power into a vacuum chamber through a dielectric partition, and In a discharge plasma processing apparatus equipped with a mechanism capable of applying a high-frequency bias for processing and using a plasma in a vacuum chamber to process the object, a high-frequency power application electrode on which the object is placed is provided. The opposing electrode provided oppositely is formed in a convex shape toward the high-frequency power application electrode, and the distance between the high-frequency power application electrode and the counter electrode is defined by the radius of the object to be treated and the radius of the convexly configured opposing electrode. It is characterized by being set based on the relationship. Preferably, the counter electrode may include a columnar protrusion extending toward the high-frequency power application electrode or a protrusion having a semi-elliptical cross section. When the opposite electrode has a columnar projection, the distance between the tip of the projection and the high-frequency power application electrode is substantially equal to the difference between the radius of the object to be processed and the radius of the opposite electrode having the projection. When the counter electrode is provided with a columnar protrusion extending toward the high-frequency power application electrode or a protrusion having a semi-elliptical cross section, the tip of the protrusion and the high-frequency power application electrode The distance of
It can be configured to be substantially equal to the difference between the radius of the object to be processed and half the radius of the base of the counter electrode having the protrusion.

【0005】[0005]

【作用】このように構成された放電プラズマ処理装置に
おいては、高周波電力印加電極すなわち基板電極と対向
電極の距離を、被処理物の半径と対向電極の半径との関
係に基づいて設定して、プラズマの拡散過程における壁
面への損失が中央部と外周部でほぼ等しくなるようにし
ているため、基板表面上におけるプラズマ密度の均一性
が得られる。基板表面上で均一になったプラズマから高
周波バイアスによって引き出されるイオンの数は均一で
あり、高均一エッチング処理やアッシング処理等の処理
を実施できるようになる。
In the discharge plasma processing apparatus configured as described above, the distance between the high-frequency power application electrode, that is, the substrate electrode and the counter electrode is set based on the relationship between the radius of the object to be processed and the radius of the counter electrode. Since the loss to the wall surface during the plasma diffusion process is made substantially equal between the central portion and the outer peripheral portion, uniformity of the plasma density on the substrate surface can be obtained. The number of ions extracted by the high-frequency bias from the plasma that has become uniform on the substrate surface is uniform, and a process such as a highly uniform etching process or an ashing process can be performed.

【0006】[0006]

【実施例】図1には本発明をエッチング装置として実施
した場合の一例を概略的に示し、1は真空チャンバー、
2は真空チャンバー1内に配置された基板電極で、高周
波電源3に接続されている。基板電極2には図示したよ
うにエッチング処理すべき基板4が装着される。真空チ
ャンバー1は排気口1aを介して図示してない排気系に連
結される。また5は基板電極2に対向して位置した対向
電極であり、この対向電極5は誘電体隔壁6を介して真
空チャンバー1の壁に取付けられている。誘電体隔壁6
の外周囲にはRFコイル7が設けられ、このRFコイル7は
誘電体隔壁6を通して真空チャンバー1内に高周波電力
を導入してプラズマを生成させるアンテナを構成してい
る。対向電極5は基板電極2に向かってのびる円柱状の
突起部5aを備え、この突起部5aの先端と基板4との距離
L1は、基板4の半径r1 と円柱状の突起部5aの半径r2
との差(r1 −r2 )に等しくなるように設定されてい
る。
FIG. 1 schematically shows an example in which the present invention is implemented as an etching apparatus, wherein 1 is a vacuum chamber,
Reference numeral 2 denotes a substrate electrode arranged in the vacuum chamber 1, which is connected to a high-frequency power supply 3. A substrate 4 to be etched is mounted on the substrate electrode 2 as shown. The vacuum chamber 1 is connected to an exhaust system (not shown) via an exhaust port 1a. Reference numeral 5 denotes a counter electrode located opposite to the substrate electrode 2, and the counter electrode 5 is attached to a wall of the vacuum chamber 1 via a dielectric partition 6. Dielectric partition 6
An RF coil 7 is provided on the outer periphery of the antenna. The RF coil 7 constitutes an antenna for generating plasma by introducing high-frequency power into the vacuum chamber 1 through the dielectric partition 6. The counter electrode 5 has a columnar projection 5a extending toward the substrate electrode 2, and the distance between the tip of the projection 5a and the substrate 4
L1 is the radius r1 of the substrate 4 and the radius r2 of the columnar projection 5a.
Is set to be equal to the difference (r1 -r2).

【0007】このように構成した図示装置を用いてエッ
チングを行なった実験例について説明する。実験条件と
しては真空チャンバー1内にArガス0.067Pa を導入し、
RFコイル7に誘導結合高周波電力 800W(13.56MHz)を
印加し、基板電極2には高周波電力600W(13.56MHz)
を印加した。対向電極5の突起部5aの先端と基板4との
距離L1を50mmとし、基板4の半径r1 と円柱状の突起部
5aの先端の半径r2 との差(r1 −r2 )もほぼ等しい
50mmとした時に、±2%のエッチング均一性が得られ
た。このとき、基板4に用いたシリコン熱酸化膜のエッ
チング速度は65nm/minであった。比較例として図1にお
いて対向電極5に円柱状の突起部5aを設けないもの(図
3に示す従来例に相当する)を用意し、実験を行なった
結果、最も良い均一性は±8%であり、アンテナすなわ
ちRFコイルの位置、上下の高周波電力の比及び圧力をパ
ラメータとして均一性の良い条件を求める実験を行なっ
たが、8%以下の均一性は得られなかった。この実験例
から図1に示す装置は従来の誘導結合型エッチング装置
に比べて均一性を大幅に改善できることが認められた。
A description will be given of an experimental example in which etching is performed using the illustrated apparatus configured as described above. As experimental conditions, 0.067 Pa of Ar gas was introduced into the vacuum chamber 1,
An inductively coupled high frequency power of 800 W (13.56 MHz) is applied to the RF coil 7, and a high frequency power of 600 W (13.56 MHz) is applied to the substrate electrode 2.
Was applied. The distance L1 between the tip of the protrusion 5a of the counter electrode 5 and the substrate 4 is set to 50 mm, and the radius r1 of the substrate 4 and the columnar protrusion are set.
The difference (r1-r2) from the radius r2 of the tip of 5a is also substantially equal
When the thickness was 50 mm, etching uniformity of ± 2% was obtained. At this time, the etching rate of the silicon thermal oxide film used for the substrate 4 was 65 nm / min. As a comparative example, one in which the columnar projection 5a was not provided on the counter electrode 5 in FIG. 1 (corresponding to the conventional example shown in FIG. 3) was prepared and an experiment was performed. As a result, the best uniformity was ± 8%. An experiment was conducted in which the conditions of good uniformity were obtained using the position of the antenna, that is, the RF coil, the ratio of the upper and lower high-frequency powers, and the pressure as parameters, but no uniformity of 8% or less was obtained. From this experimental example, it was recognized that the apparatus shown in FIG. 1 can greatly improve the uniformity as compared with the conventional inductively coupled etching apparatus.

【0008】図2には本発明をエッチング装置として実
施した場合の別例を示し、図1と対応した部分は同じ符
号で示す。この実施例では基板電極2に対向して位置し
た対向電極8に断面半楕円形状の突起部8aを設けてお
り、この場合も当然、突起部8aの先端すなわち頂部分と
基板4との距離L1は基板4の半径r1 と突起部8aの根元
部分の半径r3 の1/2 との差(r1 − 1/2・r3 )に等
しくなるように設定されている。図2に示す構造の装置
を用いて図1の場合と同様な実験例を行なった結果、こ
の場合も基板4の半径r1 と突起部8aの根元部分の半径
r3 の1/2 との差(r1− 1/2・r3 )を50mm付近にし
た時に最も良い均一性が得られた。
FIG. 2 shows another example in which the present invention is implemented as an etching apparatus, and portions corresponding to FIG. 1 are denoted by the same reference numerals. In this embodiment, a protruding portion 8a having a semi-elliptical cross section is provided on the opposing electrode 8 located opposite the substrate electrode 2. In this case, too, the distance L1 Is set to be equal to the difference between the radius r1 of the substrate 4 and 1/2 of the radius r3 of the root of the projection 8a (r1 -1 / 2.r3). An experiment similar to that of FIG. 1 was performed using the apparatus having the structure shown in FIG. 2, and as a result, also in this case, the difference between the radius r1 of the substrate 4 and 1/2 of the radius r3 of the root of the projection 8a ( The best uniformity was obtained when (r1 -1 / 2.r3) was around 50 mm.

【0009】ところで、図示実施例では基板電極に対向
して位置した対向電極として円柱状の突起部を備えたも
の及び断面半楕円形状の突起部を備えたものが用いられ
ているが、対向電極は、基板電極と対向電極との距離が
基板の半径と対向電極の半径との差にほぼ等しくなるよ
うに凸状にすればよく、従ってその形状及び寸法につい
ては任意適当に選定することができる。なお、上記実施
例では、本発明をエッチング装置として実施した場合に
ついて説明してきたが、放電プラズマを利用する他の処
理装置例えばアッシング装置及びCVD 装置においても同
様に実施でき、その場合にも図示実施例と同様の効果が
得られる。
In the illustrated embodiment, a counter electrode having a columnar projection and a projection having a semi-elliptical cross section are used as counter electrodes located opposite to the substrate electrode. May be made convex so that the distance between the substrate electrode and the counter electrode is substantially equal to the difference between the radius of the substrate and the radius of the counter electrode.Therefore, its shape and dimensions can be arbitrarily and appropriately selected. . In the above embodiment, the case where the present invention is implemented as an etching apparatus has been described. However, the present invention can be similarly implemented in other processing apparatuses using discharge plasma, for example, an ashing apparatus and a CVD apparatus. The same effect as the example can be obtained.

【0010】[0010]

【発明の効果】以上説明してきたように、本発明によれ
ば、基板電極と対向電極との距離及び基板の半径と対向
電極の半径との差または被処理物の半径と対向電極の基
部の半径の半分との差が互いにほぼ等しくなるように対
向電極を基板電極に向かって凸状に構成しているので、
生成されたプラズマの拡散による損失は中央部及び外周
部とも等しくなり、基板表面上に均一プラズマを形成す
ることができるようになる。その結果、基板表面上に形
成された均一プラズマから高周波バイアスによって引出
されるイオンの数は均一となり、高均一の処理を実施す
ることが可能となる。
As described above, according to the present invention, the distance between the substrate electrode and the counter electrode, the difference between the radius of the substrate and the radius of the counter electrode, or the difference between the radius of the object to be processed and the base of the counter electrode. Since the counter electrode is configured to be convex toward the substrate electrode so that the difference from half the radius is substantially equal to each other,
The loss due to the diffusion of the generated plasma is equal at the central portion and the outer peripheral portion, and uniform plasma can be formed on the substrate surface. As a result, the number of ions extracted from the uniform plasma formed on the substrate surface by the high-frequency bias becomes uniform, so that highly uniform processing can be performed.

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

【図1】 本発明の一実施例によるエッチング装置を示
す概略線断面図。
FIG. 1 is a schematic sectional view showing an etching apparatus according to an embodiment of the present invention.

【図2】 本発明の別の実施例を示す概略線断面図。FIG. 2 is a schematic sectional view showing another embodiment of the present invention.

【図3】 誘導結合型のエッチング装置の従来例を示す
概略線断面図。
FIG. 3 is a schematic sectional view showing a conventional example of an inductive coupling type etching apparatus.

【符号の説明】[Explanation of symbols]

1:真空チャンバー 2:基板電極 3:高周波電源 4:基板 5:対向電極 5a:円柱状突起部 6:誘電体隔壁 7:RFコイル(アンテナ) 8:対向電極 8a:断面半楕円形の突起部 1: vacuum chamber 2: substrate electrode 3: high-frequency power supply 4: substrate 5: counter electrode 5a: cylindrical protrusion 6: dielectric partition 7: RF coil (antenna) 8: counter electrode 8a: protrusion having a semi-elliptical cross section

───────────────────────────────────────────────────── フロントページの続き (72)発明者 伊藤 正博 神奈川県茅ケ崎市萩園2500番地 日本真 空技術株式会社内 (56)参考文献 特開 平7−169703(JP,A) 特開 平1−296600(JP,A) 特開 平5−226324(JP,A) 特開 平6−17253(JP,A) 特開 平4−207027(JP,A) 特表 平8−508852(JP,A) (58)調査した分野(Int.Cl.7,DB名) H01L 21/31 C23C 16/505 H01L 21/3065 H05H 1/46 ──────────────────────────────────────────────────続 き Continuation of front page (72) Inventor Masahiro Ito 2500 Hagizono, Chigasaki-shi, Kanagawa Japan Vacuum Engineering Co., Ltd. (56) References JP-A-7-169703 (JP, A) JP-A-1-296600 (JP, A) JP-A-5-226324 (JP, A) JP-A-6-17253 (JP, A) JP-A-4-207027 (JP, A) Japanese Translation of PCT Application No. 8-508852 (JP, A) ( 58) Field surveyed (Int.Cl. 7 , DB name) H01L 21/31 C23C 16/505 H01L 21/3065 H05H 1/46

Claims (6)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 誘電体隔壁を通して真空チャンバー内に
高周波電力を導入してプラズマを生成させるアンテナを
備え、被処理物を処理するために高周波バイアスを印加
できる機構を備え、真空チャンバー内でプラズマを利用
して被処理物を処理するようにした放電プラズマ処理装
置において、被処理物の載置される高周波電力印加電極
と対向して設けた対向電極を高周波電力印加電極に向っ
て凸状に構成し、高周波電力印加電極と対向電極との距
離を、被処理物の半径と凸状に構成した対向電極の半径
との関係に基づいて設定したことを特徴とする放電プラ
ズマ処理装置。
1. An antenna for generating plasma by introducing high-frequency power into a vacuum chamber through a dielectric partition, a mechanism capable of applying a high-frequency bias for processing an object to be processed is provided, and the plasma is generated in the vacuum chamber. In a discharge plasma processing apparatus configured to process an object to be processed by using the same, a counter electrode provided to face the high-frequency power application electrode on which the object is mounted is formed in a convex shape facing the high-frequency power application electrode. And a distance between the high-frequency power application electrode and the counter electrode is set based on a relationship between a radius of the object to be processed and a radius of the convex counter electrode.
【請求項2】 対向電極が高周波電力印加電極に向かっ
てのびた円柱状突起部を備えている請求項1に記載の放
電プラズマ処理装置。
2. The discharge plasma processing apparatus according to claim 1, wherein the counter electrode has a columnar projection extending toward the high-frequency power application electrode.
【請求項3】 高周波電力印加電極と対向電極との距離
を、被処理物の半径と凸状に構成した対向電極の半径と
の差に限りなく等しくするようにした請求項2に記載の
放電プラズマ処理装置。
3. The discharge according to claim 2, wherein the distance between the high-frequency power application electrode and the counter electrode is made equal to the difference between the radius of the object to be processed and the radius of the counter electrode formed in a convex shape. Plasma processing equipment.
【請求項4】 対向電極が高周波電力印加電極に向かっ
てのびた断面半楕円形の突起部を備えている請求項1に
記載の放電プラズマ処理装置。
4. The discharge plasma processing apparatus according to claim 1, wherein the counter electrode has a semi-elliptical projection extending toward the high-frequency power application electrode.
【請求項5】 高周波電力印加電極と対向電極との距離
を、被処理物の半径と凸状に構成した対向電極の基部の
半径の半分との差に限りなく等しくするようにした請求
項4に記載の放電プラズマ処理装置。
5. The distance between the high-frequency power application electrode and the counter electrode is made equal to the difference between the radius of the object to be processed and half of the radius of the base of the counter electrode formed in a convex shape. 3. The discharge plasma processing apparatus according to claim 1.
【請求項6】 対向電極が誘電体隔壁の一端に支持され
ている請求項1に記載の放電プラズマ処理装置。
6. The discharge plasma processing apparatus according to claim 1, wherein the counter electrode is supported at one end of the dielectric partition.
JP01937494A 1994-02-16 1994-02-16 Discharge plasma processing equipment Expired - Lifetime JP3357737B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP01937494A JP3357737B2 (en) 1994-02-16 1994-02-16 Discharge plasma processing equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP01937494A JP3357737B2 (en) 1994-02-16 1994-02-16 Discharge plasma processing equipment

Publications (2)

Publication Number Publication Date
JPH07230987A JPH07230987A (en) 1995-08-29
JP3357737B2 true JP3357737B2 (en) 2002-12-16

Family

ID=11997557

Family Applications (1)

Application Number Title Priority Date Filing Date
JP01937494A Expired - Lifetime JP3357737B2 (en) 1994-02-16 1994-02-16 Discharge plasma processing equipment

Country Status (1)

Country Link
JP (1) JP3357737B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8425741B2 (en) 2006-07-20 2013-04-23 Aviza Technology Limited Ion deposition apparatus having rotatable carousel for supporting a plurality of targets
US8354652B2 (en) 2006-07-20 2013-01-15 Aviza Technology Limited Ion source including separate support systems for accelerator grids
EP2044610B1 (en) 2006-07-20 2012-11-28 SPP Process Technology Systems UK Limited Plasma sources

Also Published As

Publication number Publication date
JPH07230987A (en) 1995-08-29

Similar Documents

Publication Publication Date Title
JP3942672B2 (en) Substrate processing method and substrate processing apparatus
JP3033104B2 (en) Etching method
KR100413894B1 (en) Plasma Etching Method
KR20080026042A (en) Focus ring and plasma processing device
JP3121524B2 (en) Etching equipment
KR100238573B1 (en) Method and apparatus for forming thin film
KR100381205B1 (en) Plasma CVD system and plasma CVD film deposition method
JPH10134995A (en) Plasma processing device and processing method for plasma
JP3357737B2 (en) Discharge plasma processing equipment
JPH09223685A (en) Plasma processing apparatus and plasma processing method
JPWO2008032627A1 (en) Dry etching method
US5292401A (en) Method of forming a fine pattern
KR20050091854A (en) Focus ring of semiconductor wafer manufacturing device
JP4216922B2 (en) Oxide film etching method
JPH04132220A (en) Plasma taper etching method
TWI837534B (en) Plasma processing device and processing method
JP3362093B2 (en) How to remove etching damage
US20070221332A1 (en) Plasma processing apparatus
JP3172340B2 (en) Plasma processing equipment
JP4576011B2 (en) Plasma processing equipment
JPH09172004A (en) Etching method
JPS63131519A (en) Dry etching apparatus
JP3687474B2 (en) Plasma processing equipment
JPH06120140A (en) Semiconductor manufacturing method and equipment
JP3252167B2 (en) Dry etching method

Legal Events

Date Code Title Description
R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20081004

Year of fee payment: 6

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20111004

Year of fee payment: 9

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20141004

Year of fee payment: 12

EXPY Cancellation because of completion of term