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JPH0732134B2 - Plasma equipment - Google Patents
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JPH0732134B2 - Plasma equipment - Google Patents

Plasma equipment

Info

Publication number
JPH0732134B2
JPH0732134B2 JP62164981A JP16498187A JPH0732134B2 JP H0732134 B2 JPH0732134 B2 JP H0732134B2 JP 62164981 A JP62164981 A JP 62164981A JP 16498187 A JP16498187 A JP 16498187A JP H0732134 B2 JPH0732134 B2 JP H0732134B2
Authority
JP
Japan
Prior art keywords
plasma
sample
magnetic field
magnetic
magnetic 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 - Fee Related
Application number
JP62164981A
Other languages
Japanese (ja)
Other versions
JPS63283018A (en
Inventor
誠一 中村
了 中山
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.)
Nippon Steel Corp
Original Assignee
Sumitomo Metal Industries Ltd
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 Sumitomo Metal Industries Ltd filed Critical Sumitomo Metal Industries Ltd
Priority to JP62164981A priority Critical patent/JPH0732134B2/en
Priority to EP87311451A priority patent/EP0273741B1/en
Priority to DE8787311451T priority patent/DE3774098D1/en
Priority to KR1019870015216A priority patent/KR920004912B1/en
Publication of JPS63283018A publication Critical patent/JPS63283018A/en
Priority to US07/364,585 priority patent/US5019117A/en
Priority to US07/414,511 priority patent/US5016564A/en
Publication of JPH0732134B2 publication Critical patent/JPH0732134B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はCVD(Chemical Vapor Deposition)装置、エッ
チング装置、スパッタリング装置等として用いられるプ
ラズマ装置に関するものである。
TECHNICAL FIELD The present invention relates to a plasma apparatus used as a CVD (Chemical Vapor Deposition) apparatus, an etching apparatus, a sputtering apparatus, or the like.

〔従来技術〕[Prior art]

電子サイクロトロン共鳴を利用したプラズマ装置は低ガ
ス圧で活性度の高いプラズマを生成出来、また大径のプ
ラズマ流を引き出せることから高集積半導体素子等にお
ける薄膜形成、エッチングに適用し得るものとしてその
研究,開発が進められている。
Since the plasma device using electron cyclotron resonance can generate highly active plasma at low gas pressure and can draw out a large-diameter plasma flow, its research is applicable to thin film formation and etching in highly integrated semiconductor devices etc. , Development is in progress.

第4図は薄膜形成装置として構成した従来のプラズマ装
置を示す縦断面図であり、図中31はプラズマ生成室を示
している。プラズマ生成室31は上部壁中央に石英ガラス
板31bにて封止したマイクロ波導入口31cを、また下部壁
中央には前記マイクロ波導入口31cと対向する位置にプ
ラズマ引出窓31dを夫々備えており、前記マイクロ波導
入口31cには他端を図示しない高周波発振器に接続した
導波管32の一端が接続され、またプラズマ引出窓31dに
臨ませて反応室33を配設し、更に周囲にはプラズマ生成
室31及びこれに接続した導波管32の一端部にわたってこ
れらを囲繞する態様でこれらと同心状に励磁コイル34を
配設してある。
FIG. 4 is a vertical cross-sectional view showing a conventional plasma apparatus configured as a thin film forming apparatus, and 31 in the figure shows a plasma generation chamber. The plasma generation chamber 31 is provided with a microwave introduction port 31c sealed with a quartz glass plate 31b at the center of the upper wall, and a plasma extraction window 31d at a position facing the microwave introduction port 31c at the center of the lower wall. One end of a waveguide 32 whose other end is connected to a high-frequency oscillator (not shown) is connected to the microwave introduction port 31c, and a reaction chamber 33 is disposed so as to face the plasma extraction window 31d, and plasma is further generated in the surroundings. An exciting coil 34 is arranged concentrically with the chamber 31 and one end of the waveguide 32 connected thereto so as to surround them.

反応室33内には円盤形の載置台37が配設され、その上に
は円板形をなすウェーハ等の試料Sがそのまま、又は静
電吸着等の手段にて着脱可能に載置され、更に反応室33
の下部壁には図示しない排気装置に連なる排気口33aが
開口されている。31g,33gは原料ガス供給管である。
A disk-shaped mounting table 37 is provided in the reaction chamber 33, and a sample S such as a disk-shaped wafer is mounted on the mounting table 37 as it is or detachably by means such as electrostatic adsorption. Further reaction chamber 33
An exhaust port 33a connected to an exhaust device (not shown) is opened in the lower wall of the. 31g and 33g are raw material gas supply pipes.

而してこのような薄膜形成装置にあっては、所要の真空
度に設定したプラズマ生成室31,反応室33内に原料ガス
を供給し、励磁コイル34にて磁界を形成しつつプラズマ
生成室31内にマイクロ波を導入してプラズマを生成さ
せ、生成させたプラズマを励磁コイル34にて形成される
プラズマ引出窓31d前方の反応室33側に向かうに従い磁
束密度が低下する発散磁界によってプラズマ生成室31か
らプラズマ引出窓31dを経て反応室33内の載置台37の試
料S周辺に導出し、試料S表面でプラズマ流中のイオ
ン,ラジカル粒子による表面反応を生起させ試料S表面
に成膜するようになっている(特開昭56-155535号)。
Thus, in such a thin film forming apparatus, the source gas is supplied into the plasma generation chamber 31 and the reaction chamber 33 which are set to a required degree of vacuum, and the excitation coil 34 forms a magnetic field while the plasma generation chamber is formed. Plasma is generated by introducing microwave into the plasma 31, and the generated plasma is generated by a divergent magnetic field whose magnetic flux density decreases toward the reaction chamber 33 side in front of the plasma extraction window 31d formed by the excitation coil 34. It is led out from the chamber 31 through the plasma extraction window 31d to the periphery of the sample S on the mounting table 37 in the reaction chamber 33, and a surface reaction is caused by the ions and radical particles in the plasma flow on the sample S surface to form a film on the sample S surface. (Japanese Patent Laid-Open No. 56-155535).

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

ところで上述した如き従来のプラズマ装置にあってはプ
ラズマ生成室31で発生せしめられたプラズマは励磁コイ
ル34によって形成される発散磁界の磁力線に沿ってプラ
ズマ引出窓31dを経て反応室33内の試料S側に引き出さ
れる。
By the way, in the conventional plasma apparatus as described above, the plasma generated in the plasma generation chamber 31 passes through the plasma extraction window 31d along the magnetic field lines of the divergent magnetic field formed by the exciting coil 34 and passes through the sample S in the reaction chamber 33. Pulled out to the side.

前記プラズマは、プラズマ生成室31内で一様には発生せ
ず、プラズマ生成室31中心部でプラズマ密度がより高く
なるように発生するために、そのプラズマ生成室31内の
むらが発散磁界によりそのまま試料Sに向かって拡大投
影されてしまうという現象が認められる。従って、発散
磁界より引き出されたプラズマのプラズマ密度分布は試
料S中央部で高く、周縁部で低くなって、試料S内にお
ける堆積速度に差が生じ、膜厚の不均一が避けられない
という問題があった。
The plasma is not uniformly generated in the plasma generation chamber 31, but is generated so that the plasma density becomes higher in the central portion of the plasma generation chamber 31, so that the unevenness in the plasma generation chamber 31 remains unchanged due to the divergent magnetic field. A phenomenon that the image is enlarged and projected toward the sample S is recognized. Therefore, the plasma density distribution of the plasma extracted from the divergent magnetic field is high in the central portion of the sample S and low in the peripheral portion, which causes a difference in the deposition rate in the sample S, and the nonuniformity of the film thickness cannot be avoided. was there.

このような膜厚、或いはエッチング深さの不均一性は薄
膜形成装置においてのみならず、エッチング装置、スパ
ッタ薄膜形成装置(特開昭59-47728号)として用いる場
合においても処理速度がばらつく同様な現象が認められ
ている。
Such non-uniformity of the film thickness or the etching depth varies not only in the thin film forming apparatus but also in the case where the film is used as an etching apparatus or a sputtered thin film forming apparatus (Japanese Patent Laid-Open No. 59-47728). The phenomenon is acknowledged.

本発明はかかる事情に鑑みなされたものであって、その
目的とするところは表面での磁束密度分布を均一化し、
プラズマ密度を均一にし、均一な厚さの成膜、或いは均
一なエッチング処理を行い得るようにしたプラズマ装置
を提供するにある。
The present invention has been made in view of such circumstances, the object is to make the magnetic flux density distribution on the surface uniform,
It is another object of the present invention to provide a plasma device having a uniform plasma density and capable of performing uniform film formation or uniform etching.

〔問題点を解決するための手段〕[Means for solving problems]

本発明に係るプラズマ装置は電子サイクロトロン共鳴を
利用してプラズマを発生させ、これを磁界を利用してプ
ラズマ引出窓から試料の載置台を備える試料室に導出す
るようにしたプラズマ装置において、前記載置台の試料
に対しプラズマ引出窓と反対側に、試料周縁部の磁束密
度が中央部のそれより高い磁界を生成する磁界生成器を
配設し、該磁界生成器は、前記試料表面でのプラズマ密
度を均一にすべく、前記試料の直径と略等しいか又はこ
れよりも大きい外径を有する円筒形の磁性体と、該磁性
体の周囲に同心に配設されたコイルとで構成したことを
特徴とする。
The plasma device according to the present invention is a plasma device in which plasma is generated using electron cyclotron resonance, and this is led out from a plasma extraction window to a sample chamber provided with a sample mounting table by using a magnetic field. A magnetic field generator for generating a magnetic field having a higher magnetic flux density in the peripheral portion of the sample than that in the central portion is arranged on the opposite side of the plasma drawing window with respect to the sample on the mounting table, and the magnetic field generator generates plasma on the sample surface. In order to make the density uniform, it is composed of a cylindrical magnetic body having an outer diameter substantially equal to or larger than the diameter of the sample, and a coil arranged concentrically around the magnetic body. Characterize.

〔作用〕[Action]

本発明は円筒形の磁性体と、磁性体の周囲に同心に配設
されたコイルとからなる磁界生成器により、試料の周縁
部における磁束密度が中央部に対して相対的に高く、従
ってこれに対して引き出されるプラズマは、プラズマ生
成室31の周縁部で低密度であった部分が試料S表面では
密度が高まり、逆にプラズマ生成室31の中央部で高密度
であった部分が試料S表面では密度が低くなり、この結
果試料S表面上でプラズマ密度分布が均一化される。こ
のため従来は不均一性であった成膜速度,エッチング速
度等の処理速度が均一化される。
The present invention uses a magnetic field generator composed of a cylindrical magnetic body and a coil arranged concentrically around the magnetic body, so that the magnetic flux density at the peripheral portion of the sample is relatively high relative to the central portion, and With respect to the plasma drawn out, the portion having a low density in the peripheral portion of the plasma generation chamber 31 has a high density on the surface of the sample S, and conversely, the portion having a high density in the central portion of the plasma generation chamber 31 has the sample S. The density becomes low on the surface, and as a result, the plasma density distribution is made uniform on the surface of the sample S. Therefore, the processing speed such as the film forming speed and the etching speed, which have been non-uniform in the past, is made uniform.

〔実施例〕〔Example〕

以下本発明を薄膜形成装置として構成した実施例につき
図面に基づき具体的に説明する。第1図は本発明に係る
プラズマ装置(以下本発明装置という)の縦断面図であ
り、図中1はプラズマ生成室、2は導波管、3は試料S
に対し成膜を施す試料室たる反応室、4は励磁コイルを
示している。
An embodiment in which the present invention is configured as a thin film forming apparatus will be specifically described below with reference to the drawings. FIG. 1 is a longitudinal sectional view of a plasma device according to the present invention (hereinafter referred to as the device of the present invention), in which 1 is a plasma generation chamber, 2 is a waveguide, and 3 is a sample S.
On the other hand, a reaction chamber 4 which is a sample chamber for film formation shows an exciting coil.

プラズマ生成室1は上部壁中央には石英ガラス板1bで閉
鎖されたマイクロ波導入口1cを備え、また下部壁中央に
は前記マイクロ波導入口1cと対向する位置に円形のプラ
ズマ引出窓1dを備えており、前記マイクロ波導入口1cに
は導波管2の一端部が接続され、またプラズマ引出窓1d
にはこれに臨ませて反応室3が配設され、更に周囲には
プラズマ生成室1及びこれに連結された導波管2の一端
部にわたって励磁コイル4が周設せしめられている。
The plasma generation chamber 1 has a microwave introduction port 1c closed by a quartz glass plate 1b at the center of the upper wall, and a circular plasma extraction window 1d at a position facing the microwave introduction port 1c at the center of the lower wall. One end of the waveguide 2 is connected to the microwave introduction port 1c, and the plasma extraction window 1d
A reaction chamber 3 is disposed so as to face this, and an exciting coil 4 is provided around the plasma generating chamber 1 and one end of a waveguide 2 connected to the plasma generating chamber 1.

導波管2の他端部は図示しない高周波発振器に接続され
ており、発せられたマイクロ波をマイクロ波導入口1cか
らプラズマ生成室1内に導入するようにしてある。励磁
コイル4は図示しない直流電源に接続されており、直流
電流の通流によってプラズマ生成室1内にマイクロ波の
導入によりプラズマを生成し得るよう磁界を形成すると
共に、反応室3側に向けて磁束密度が低くなる発散磁界
を形成し、プラズマ生成室1内に生成されたプラズマを
反応室3内に導出せしめるようになっている。
The other end of the waveguide 2 is connected to a high-frequency oscillator (not shown) so that the emitted microwave is introduced into the plasma generation chamber 1 through the microwave introduction port 1c. The exciting coil 4 is connected to a DC power source (not shown), forms a magnetic field so that plasma can be generated by introducing microwaves into the plasma generation chamber 1 by flowing a DC current, and the excitation coil 4 is directed toward the reaction chamber 3 side. A divergent magnetic field that lowers the magnetic flux density is formed so that the plasma generated in the plasma generation chamber 1 can be led out to the reaction chamber 3.

反応室3内にはその下部中央であって、プラズマ引出窓
1dと対向する位置に載置台7が配設され、その上には円
板形をなすウェーハ等の試料Sがそのまま、又は静電吸
着等の手段にて着脱可能に載置されるようにしてあり、
また底壁には図示しない排気装置に連なる排気口3aを開
口してある。1g,3gは原料ガス供給管である。
At the center of the lower part of the reaction chamber 3, there is a plasma extraction window.
A mounting table 7 is arranged at a position facing 1d, and a sample S such as a disk-shaped wafer is mounted on the mounting table 7 as it is or detachably by means such as electrostatic adsorption. Yes,
Further, the bottom wall is provided with an exhaust port 3a which communicates with an exhaust device (not shown). 1g and 3g are raw material gas supply pipes.

そして本発明装置にあっては前記載置台7の下部に、円
筒形に形成された磁性体5がプラズマ引出窓1d、載置台
7及びこの上に載置される試料Sと略同心に配設されて
いる。この磁性体5の外径Dは試料Sの直径と略等しい
か、又はこれよりも大きく設定され、また内径dは零以
外、即ち0<d<Dに設定されている。
In the apparatus of the present invention, the cylindrical magnetic body 5 is disposed below the mounting table 7 substantially concentrically with the plasma extraction window 1d, the mounting table 7 and the sample S mounted thereon. Has been done. The outer diameter D of the magnetic body 5 is set to be substantially equal to or larger than the diameter of the sample S, and the inner diameter d is set to a value other than zero, that is, 0 <d <D.

第2図は上述した如き円板形の試料Sと外径Dの円筒形
をなす磁性体5を用いた場合の磁力線の様子を示す説明
図であり、励磁コイル4にて形成される発散磁界の磁力
線は磁性体5に引き寄せられる。すなわち、磁性体5の
外側に拡がった磁力線は内側へ引き戻され、磁性体5の
内側の磁力線は外側に押し拡げられる結果プラズマ生成
室31から引き出されたプラズマの試料S表面での密度分
布はこれに対応して均一化される。
FIG. 2 is an explanatory diagram showing a state of magnetic force lines when the disk-shaped sample S and the cylindrical magnetic body 5 having the outer diameter D as described above are used, and the divergent magnetic field formed by the exciting coil 4 is shown. The magnetic lines of force are attracted to the magnetic body 5. That is, the magnetic field lines spreading outside the magnetic body 5 are pulled back inward, and the magnetic field lines inside the magnetic body 5 are pushed outward, so that the density distribution of the plasma drawn from the plasma generation chamber 31 on the surface of the sample S is Is equalized corresponding to.

以下これにつき更に詳しく説明する。This will be described in more detail below.

本発明において重要なことは試料周縁部の磁束密度が中
央部より高い磁界を生成する磁界生成器、つまり上記実
施例では円筒型の磁性体5を用いることが重要である。
What is important in the present invention is that it is important to use a magnetic field generator that generates a magnetic field having a higher magnetic flux density in the peripheral portion of the sample than in the central portion, that is, the cylindrical magnetic body 5 in the above embodiment.

例えば特公昭58-13627号には本願発明と同様にマイクロ
波とによってプラズマを発生させるエッチング装置が記
されており、試料に対し、上記磁界を発生させるコイル
又はプラズマ引出窓と反対側に磁石を設けてミラー磁場
を形成することとしている。第6図はミラー磁場を形成
した場合の磁力線の様子を示す模式図である。図におい
て61は発散磁界を形成するコイル、62はミラー磁場を形
成する磁石である。このようなミラー磁場は磁石62の存
在によってコイル61によって生成された磁束が発散せず
に収束するものの、磁束密度は中央部において高く、周
縁部において低い状態のままであり、この磁場内に試料
を置く場合はプラズマが無駄なく利用できるとしても試
料表面でのプラズマ密度の均一化は望めないのである。
For example, Japanese Examined Patent Publication No. 58-13627 describes an etching device for generating a plasma by a microwave as in the present invention, and a magnet is provided on the opposite side of a coil for generating the magnetic field or a plasma extraction window from the sample. It is provided to form a mirror magnetic field. FIG. 6 is a schematic diagram showing a state of magnetic force lines when a mirror magnetic field is formed. In the figure, 61 is a coil that forms a divergent magnetic field, and 62 is a magnet that forms a mirror magnetic field. In such a mirror magnetic field, although the magnetic flux generated by the coil 61 converges without diverging due to the presence of the magnet 62, the magnetic flux density is high in the central part and remains low in the peripheral part, and the sample is placed in this magnetic field. However, even if the plasma can be used without waste, it is not possible to make the plasma density uniform on the sample surface.

第7図は試料中心からの距離r(cm)(第6図参照)と
載置台7上における載置台に垂直方向の成分である磁束
密度Bz分布との関係を発散磁界(破線),ミラー磁界
(1点斜線)及び本発明の磁界生成器による磁界(実
線)について記したものである。この図から明らかな如
く、本発明装置は試料周縁部を中央部より高くすること
で、発散磁界又はミラー磁場ではプラズマ生成室内のプ
ラズマ密度分布(周縁部が低い)がそのまま投影される
だけであるのを補正することが可能なのである。
FIG. 7 shows the relationship between the distance r (cm) from the center of the sample (see FIG. 6) and the magnetic flux density Bz distribution, which is a component in the direction perpendicular to the mounting table on the mounting table 7, showing the divergent magnetic field (broken line) and the mirror magnetic field. (One-dot diagonal line) and the magnetic field (solid line) by the magnetic field generator of the present invention are described. As is clear from this figure, in the apparatus of the present invention, by making the peripheral portion of the sample higher than the central portion, the plasma density distribution (the peripheral portion is low) in the plasma generating chamber is projected as it is in the divergent magnetic field or the mirror magnetic field. Can be corrected.

第3図は本発明装置において用いる磁性体の他の構成を
示す模式的断面図であり、円筒形をなす磁性体5の外周
面に隙間なく細い絶縁被覆された導電線6を密に多数回
巻着せしめ、その端部間には図示しない直流電源を接続
してあり、必要な大きさの直流電流を通流して試料S表
面に対する磁束密度分布を微調節し得るようにしてあ
る。
FIG. 3 is a schematic cross-sectional view showing another configuration of the magnetic body used in the device of the present invention, in which a thin insulating coated conductive wire 6 is closely packed many times on the outer peripheral surface of the cylindrical magnetic body 5. It is wound around, and a DC power supply (not shown) is connected between its ends so that a DC current of a required magnitude can be passed to finely adjust the magnetic flux density distribution on the surface of the sample S.

なお絶縁被覆された導電線6は磁性体5の外周面に直接
巻き付ける代わりに磁性体5の周囲にリング形に配設し
てもよい。他の構成は第1,2図に示す磁性体と実質的に
同じである。
The electrically conductive wire 6 coated with insulation may be arranged in a ring shape around the magnetic body 5 instead of being wound directly on the outer peripheral surface of the magnetic body 5. The other structure is substantially the same as that of the magnetic body shown in FIGS.

また上述の各実施例では、磁性体5を載置台7の下部に
配設した構成を示したが、試料Sの下であればどのよう
な位置でもよく磁性体5を載置台7上に配設し、或いは
磁性体5と載置台7とを一体的に構成し、或いは磁性体
5が載置台7を兼ねるよう構成してもよい。
Further, in each of the above-described embodiments, the magnetic body 5 is arranged below the mounting table 7, but the magnetic body 5 may be arranged on the mounting table 7 at any position below the sample S. Alternatively, the magnetic body 5 and the mounting table 7 may be integrally formed, or the magnetic body 5 may also serve as the mounting table 7.

上述した如き本発明装置と第4図に示す従来装置とにつ
いて夫々プラズマ生成室1へO2ガスを、また反応室3へ
SiH4ガスを夫々原料ガスとして導入してプラズマを発生
させ、これを載置台7上の直径5インチのSiウェーハ上
に堆積せしめ、その膜厚分布のばらつきを測定した結
果、従来装置では±10%あったが、本発明装置では±5
%に低減することが出来た。
Regarding the apparatus of the present invention as described above and the conventional apparatus shown in FIG. 4, O 2 gas was supplied to the plasma generation chamber 1 and to the reaction chamber 3 respectively.
SiH 4 gas was introduced as a source gas to generate plasma, which was deposited on a Si wafer having a diameter of 5 inches on the mounting table 7, and the variation in the film thickness distribution was measured. %, But ± 5 with the device of the present invention
Could be reduced to%.

なお膜厚分布は下式によって求めた。The film thickness distribution was calculated by the following formula.

〔効果〕 以上の如く本発明装置にあっては、試料に対し、プラズ
マ引出窓と反対側に円筒形の磁性体とその周囲に同心に
配設されたコイルによって、試料室側に向けて形成され
る発散磁界の磁力線のうち、試料の周縁部又はその近傍
の磁力線が試料周縁部と交叉する向き、つまり内外方向
に湾曲せしめられ、試料周縁部の磁束密度が高められ、
試料表面での磁束密度分布が改善され、均一な厚さの成
膜等の処理を行い得るなど、本発明は優れた効果を奏す
るものである。
[Effects] As described above, in the device of the present invention, the sample is formed toward the sample chamber side by the cylindrical magnetic body on the side opposite to the plasma drawing window and the coil concentrically arranged around the magnetic body. Among the magnetic field lines of the divergent magnetic field, the magnetic field lines in the peripheral portion of the sample or in the vicinity thereof are curved in a direction intersecting the sample peripheral portion, that is, inward and outward directions, and the magnetic flux density in the peripheral portion of the sample is increased,
The present invention has excellent effects such that the magnetic flux density distribution on the surface of the sample is improved and the film can be formed into a film having a uniform thickness.

【図面の簡単な説明】 第1図は本発明装置の縦断面図、第2図は本発明装置に
おける磁力線を示す説明図、第3図は本発明装置に用い
る磁性体の他の構成を示す拡大断面図、第4図は従来装
置の縦断面図、第5図は従来装置におけるプラズマ引出
用の発散磁界の磁力線と試料との関係を示す説明図、第
6図はミラー磁場の説明図、第7図は各種の磁場におけ
る磁束密度分布図である。 1……プラズマ生成室、2……導波管、3……反応室、
4……励磁コイル、5……磁性体、6……導電線、7…
…載置台、S……試料
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a vertical cross-sectional view of the device of the present invention, FIG. 2 is an explanatory view showing lines of magnetic force in the device of the present invention, and FIG. 3 shows another structure of a magnetic body used in the device of the present invention. FIG. 4 is an enlarged cross-sectional view, FIG. 4 is a vertical cross-sectional view of a conventional apparatus, FIG. 5 is an explanatory view showing a relationship between a magnetic field line of a diverging magnetic field for plasma extraction in the conventional apparatus and a sample, FIG. 6 is an explanatory view of a mirror magnetic field, FIG. 7 is a magnetic flux density distribution diagram in various magnetic fields. 1 ... Plasma generation chamber, 2 ... Waveguide, 3 ... Reaction chamber,
4 ... Excitation coil, 5 ... Magnetic material, 6 ... Conductive wire, 7 ...
… Mounting table, S… Sample

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】電子サイクロトロン共鳴を利用してプラズ
マを発生させ、これを磁界を利用してプラズマ引出窓か
ら試料の載置台を備える試料室に導出するようにしたプ
ラズマ装置において、 前記載置台の試料に対しプラズマ引出窓と反対側に、試
料周縁部の磁束密度が中央部のそれより高い磁界を生成
する磁界生成器を配設し、該磁界生成器は、前記試料表
面でのプラズマ密度を均一にすべく、前記試料の直径と
略等しいか又はこれよりも大きい外径を有する円筒形の
磁性体と、該磁性体の周囲に同心に配設されたコイルと
で構成したことを特徴とするプラズマ装置。
1. A plasma apparatus in which plasma is generated by utilizing electron cyclotron resonance, and the plasma is led out from a plasma extraction window to a sample chamber provided with a sample table by using a magnetic field. A magnetic field generator for generating a magnetic field having a higher magnetic flux density in the peripheral portion of the sample than that in the central portion is arranged on the side opposite to the plasma extraction window with respect to the sample, and the magnetic field generator controls the plasma density on the sample surface. In order to make it uniform, it is composed of a cylindrical magnetic body having an outer diameter substantially equal to or larger than the diameter of the sample, and a coil concentrically arranged around the magnetic body. Plasma device.
JP62164981A 1986-12-29 1987-06-30 Plasma equipment Expired - Fee Related JPH0732134B2 (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP62164981A JPH0732134B2 (en) 1986-12-29 1987-06-30 Plasma equipment
EP87311451A EP0273741B1 (en) 1986-12-29 1987-12-24 Plasma apparatus
DE8787311451T DE3774098D1 (en) 1986-12-29 1987-12-24 PLASMA UNIT.
KR1019870015216A KR920004912B1 (en) 1986-12-29 1987-12-29 Plasma device
US07/364,585 US5019117A (en) 1986-12-29 1989-06-12 Plasma apparatus
US07/414,511 US5016564A (en) 1986-12-29 1989-09-29 Plasma apparatus

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP30956086 1986-12-29
JP61-309560 1986-12-29
JP62164981A JPH0732134B2 (en) 1986-12-29 1987-06-30 Plasma equipment

Publications (2)

Publication Number Publication Date
JPS63283018A JPS63283018A (en) 1988-11-18
JPH0732134B2 true JPH0732134B2 (en) 1995-04-10

Family

ID=26489888

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62164981A Expired - Fee Related JPH0732134B2 (en) 1986-12-29 1987-06-30 Plasma equipment

Country Status (1)

Country Link
JP (1) JPH0732134B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0521874Y2 (en) * 1989-12-01 1993-06-04

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61213377A (en) * 1985-03-18 1986-09-22 Hitachi Ltd Method and apparatus for plasma deposition

Also Published As

Publication number Publication date
JPS63283018A (en) 1988-11-18

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