JPH02139924A - Plasma reaction device - Google Patents

Plasma reaction device

Info

Publication number
JPH02139924A
JPH02139924A JP63292419A JP29241988A JPH02139924A JP H02139924 A JPH02139924 A JP H02139924A JP 63292419 A JP63292419 A JP 63292419A JP 29241988 A JP29241988 A JP 29241988A JP H02139924 A JPH02139924 A JP H02139924A
Authority
JP
Japan
Prior art keywords
plasma
reaction chamber
sample
magnetic
chamber
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP63292419A
Other languages
Japanese (ja)
Inventor
Masahiro Shimizu
雅裕 清水
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP63292419A priority Critical patent/JPH02139924A/en
Publication of JPH02139924A publication Critical patent/JPH02139924A/en
Pending legal-status Critical Current

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  • ing And Chemical Polishing (AREA)
  • Drying Of Semiconductors (AREA)
  • Plasma Technology (AREA)

Abstract

PURPOSE:To improve uniformity and processing configuration of etching inside a sample surface by providing an inside and an outside of a reaction chamber with a magnetic coil which scans a magnetic line of nonuniform magnetic field which is generated by another magnetic coil provided at a periphery of a plasma generating chamber. CONSTITUTION:After interior of a plasma generating chamber 1 and a reaction chamber 5 is exhausted, material gas is introduced to the reaction chamber to keep a specified gas pressure. Then, micro wave is introduced from a microwave introduction port 4. ECR plasma which is generated in the generating chamber 1 through mutual operation of an nonuniform magnetic field generated by a magnetic coil 2 and the microwave is transferred along and by a magnetic line 9 of a part of nonuniform magnetic field produced inside the reaction chamber 5, and introduced to the reaction chamber 5. In the reaction chamber 5, the magnetic line 9 is scanned by a magnetic coil 2A; therefore, ECR plasma attains a surface of a sample 8 and proceeds etching while an incident angle to a position of the surface of the sample 8 changes successively according thereto. As a result, a processed thin film 8b of almost vertical etching shape can be acquired.

Description

【発明の詳細な説明】 [産業上の利用分野コ この発明は、プラズマ反応装置に関するものであり、特
に半導体装置を製造する際にエツチング工程などで使用
されるプラズマ反応装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a plasma reaction apparatus, and more particularly to a plasma reaction apparatus used in an etching process and the like when manufacturing semiconductor devices.

「従来の技術」 第4図は、電子サイクロトロン共鳴(Electron
Cyclotron Re5onance、 ECR)
を利用したこの種の従来のプラズマ反応装置を示す断面
図である。図において、(1)は高密度のガスプラズマ
を発生するプラズマ発生室、(2)はこのプラズマ発生
室(1)の周囲に設けられて、後述のECRを惹起させ
る不均一磁界を発生する磁気コイル、(3)はプラズマ
発生室(1)の上部に設けられ、高密度ガスプラズマの
原料ガスを導入するガス導入口、(4)はプラズマ発生
室(1)の上部に設けられ、磁気コイル(2)によって
発生された不均一磁界と相互作用し、ECRの原理に従
って螺旋運動する電子をプラズマ発生室(1)内に惹起
するマイクロ波を導入するマイクロ波導入口、(5)は
プラズマ発生室(1)内でECRにより発生した螺旋運
動電子などの衝突により発生した高密度ガスプラズマを
上述の不均一磁場に従って導入し、後述のエツチング加
工を行わせる反応室、(6)はこの反応室(5)の下部
に設けられ、プラズマ発主室(1)に導入された原料ガ
スを所定のガス圧力に保持するため原料ガスを適切に排
気する排気口、(7)は反応室(6)内に設置され、被
加工試料(8)を保持する試料保持台、そして(9)は
不均一磁界を示す磁力線である。
"Prior art" Figure 4 shows electron cyclotron resonance (Electron resonance).
Cyclotron Re5onance, ECR)
1 is a cross-sectional view showing a conventional plasma reactor of this type using a plasma reactor. In the figure, (1) is a plasma generation chamber that generates high-density gas plasma, and (2) is a magnetic field provided around this plasma generation chamber (1) that generates a nonuniform magnetic field that causes ECR, which will be described later. The coil (3) is provided at the top of the plasma generation chamber (1) and is a gas inlet for introducing raw material gas for high-density gas plasma.The coil (4) is provided at the top of the plasma generation chamber (1) and is a magnetic coil. (2) is a microwave introduction port that introduces microwaves that interact with the non-uniform magnetic field generated by the plasma generating chamber (1) and cause electrons to move spirally according to the principle of ECR into the plasma generating chamber; (5) is a plasma generating chamber; (1) A reaction chamber in which a high-density gas plasma generated by collisions of spirally moving electrons generated by ECR is introduced in accordance with the above-mentioned inhomogeneous magnetic field to perform the etching process described later; (6) is this reaction chamber ( 5) is an exhaust port provided at the bottom of the plasma generator chamber (1) to properly exhaust the source gas introduced into the plasma generation chamber (1) in order to maintain it at a predetermined gas pressure. A sample holder is installed on the substrate and holds a sample to be processed (8), and (9) is a line of magnetic force indicating a non-uniform magnetic field.

第5図は第4図に示した従来のプラズマ反応装置による
試料(8)の加工形状を示す拡大断面図であり、図にお
いて、(8a)は半導体基板、(8b)はこの半導体基
板(8a)上の被加工薄膜である。
FIG. 5 is an enlarged sectional view showing the processed shape of the sample (8) using the conventional plasma reaction apparatus shown in FIG. ) is the thin film to be processed.

従来のプラズマ反応装置は上述したように構成され、そ
の動作は次のようになる。
A conventional plasma reactor is constructed as described above, and its operation is as follows.

ガス導入口(3)からプラズマ発生室(1)内に反応性
の原料ガスを導入する。また、排気口(6)から排気を
行い、プラズマ発生室(1)内を所定のガス圧力に保持
する。次に、マイクロ波導入口(4)から例えば2.4
5GIlzのマイクロ波を導入する。ここで、磁気コイ
ル(2)を励磁して不均一磁界を発生させ、マイクロ波
との相互作用により原料ガスにECRを惹起させ、これ
によりプラズマ発生室(1)内に生じた螺旋運動電子な
どのプラズマ成分同士の衝突により、高密度のガスプラ
ズマが生成される。このガスプラズマは不均一磁界の磁
力線(9)に沿って反応室(5)に導かれ、ここで試料
(8)の表面に形成された被加工薄膜(8b)をエツチ
ング処理する。
A reactive raw material gas is introduced into the plasma generation chamber (1) through the gas introduction port (3). Further, exhaust is performed from the exhaust port (6) to maintain the inside of the plasma generation chamber (1) at a predetermined gas pressure. Next, from the microwave inlet (4), for example, 2.4
Introducing 5GIlz microwave. Here, the magnetic coil (2) is excited to generate a non-uniform magnetic field, and ECR is induced in the raw material gas by interaction with the microwave, thereby causing spiral movement electrons etc. generated in the plasma generation chamber (1). A high-density gas plasma is generated by the collision of the plasma components. This gas plasma is guided into the reaction chamber (5) along the lines of magnetic force (9) of the non-uniform magnetic field, where it etches the thin film to be processed (8b) formed on the surface of the sample (8).

[発明が解決しようとする課題] 従来のプラズマ反応装置は、プラズマ発生室(1)から
試料(8)の方向に向けて磁力線(9)が発散するよう
になっており、いわゆる発散磁場によりプラズマを試料
(8)の表面に輸送するように構成されている。このた
め、試料(8)の表面に達する反応性イオンの入射角お
よびエネルギーは試料(8)の表面位置により異なるこ
とになる。
[Problems to be Solved by the Invention] In the conventional plasma reaction device, lines of magnetic force (9) diverge from the plasma generation chamber (1) toward the sample (8), and the so-called divergent magnetic field causes the plasma to is configured to transport to the surface of the sample (8). Therefore, the incident angle and energy of the reactive ions reaching the surface of the sample (8) differ depending on the surface position of the sample (8).

この結果、試料(8)の周辺部においてエツチングの形
状が垂直性を失い、第5図に示したように非対称に加工
されるという問題点があった。
As a result, there was a problem in that the etched shape lost its verticality in the peripheral area of the sample (8), resulting in asymmetrical etching as shown in FIG.

この発明は、このような問題点を解決するためになされ
たもので、試料面内におけるエツチングの均一性および
加工形状を向上させることのできるプラズマ反応装置を
提供することを目的とする。
The present invention has been made to solve these problems, and an object of the present invention is to provide a plasma reaction apparatus that can improve the uniformity of etching within the surface of a sample and the processed shape.

[課題を解決するための手段] この発明に係るプラズマ反応装置は、プラズマ発生室の
周囲に設けられた磁気コイルが発生する不均一磁界の磁
力線を走査する他の磁気コイルを反応室の内部または外
部に設けたものである。
[Means for Solving the Problems] A plasma reaction apparatus according to the present invention has a magnetic coil provided around a plasma generation chamber that scans lines of magnetic force of a nonuniform magnetic field generated by a magnetic coil provided inside the reaction chamber or inside the reaction chamber. It is installed outside.

[作 用] この発明においては、磁気コイルの発生する不均一磁界
の磁力線を他の磁気コイルが走査して変化させるように
したので、試料表面に入射衝突する高密度プラズマ粒子
の入射角度を変化させて被加工試料の加工形状を垂直に
することができる。
[Function] In this invention, the lines of magnetic force of the nonuniform magnetic field generated by the magnetic coil are scanned and changed by other magnetic coils, so that the angle of incidence of high-density plasma particles that collide with the sample surface is changed. This allows the machining shape of the workpiece to be made vertical.

[実施例] 第1図はこの発明の一実施例を示す断面図、第2図は他
の実施例を示す断面図、そして第3図は各実施例により
エツチングした試料の加工形状を示す拡大断面図である
。第1図のプラズマ反応装置が第4図のプラズマ反応装
置と異なる唯一の点は、プラズマ発生室(1)から発散
する不均一磁界を走査する他の磁気コイル(2^)を反
応室(6)内に設けたことである。
[Example] Fig. 1 is a sectional view showing one embodiment of the present invention, Fig. 2 is a sectional view showing another embodiment, and Fig. 3 is an enlarged view showing the processed shape of a sample etched according to each embodiment. FIG. The only difference between the plasma reactor shown in FIG. 1 and the plasma reactor shown in FIG. ).

第2図のプラズマ反応装置は、第1図の実施例に、更に
試料(8)面上に他の磁気コイル(2A)の走査と同期
するじゃへいtli (10)を設けたものである。
The plasma reactor shown in FIG. 2 is the same as the embodiment shown in FIG. 1, but further provided with a Jaheitli (10) on the surface of the sample (8) which is synchronized with the scanning of another magnetic coil (2A).

上述したように構成されたプラズマ反応装置は次のよう
に動作する。
The plasma reactor configured as described above operates as follows.

第1図に示したように、プラズマ発生室(1)と反応室
(5)の内部と排気口(4)を通して十分排気する。そ
の後、ガス導入口(3)から反応性の原料ガスを導入し
、所定のガス圧力に保持する。次に、マイクロ波導入口
(4)から例えば2.45Gllzのマイクロ波を導入
する。磁気コイル(2)によって発生された不均一磁界
とマイクロ波との相互作用によりプラズマ発生室(1)
にECRの原理に従って高密度ECRプラズマが発生す
る。このECRプラズマは、反応室(5)内の発散する
不均一磁界の一部の磁力線(9)により、これに沿って
輸送され、反応室(5)に導入される。反応室(5)で
は、磁力線(9)が磁気コイル(2人)によって走査さ
れているので、入射したECRプラズマは試料(8)面
の位置に応じてそれに対する入射角が連続的に変化しな
がら試料(8)面に達してエツチングを進行させる。こ
の結果、第3図に示したように、垂直に近いエツチング
形状の被加工薄膜(8b)が得られる。
As shown in FIG. 1, the plasma generation chamber (1) and reaction chamber (5) are sufficiently evacuated through the exhaust port (4). Thereafter, a reactive raw material gas is introduced from the gas inlet (3) and maintained at a predetermined gas pressure. Next, a microwave of 2.45 Gllz, for example, is introduced from the microwave inlet (4). Plasma generation chamber (1) is generated by the interaction between the microwave and the non-uniform magnetic field generated by the magnetic coil (2).
High-density ECR plasma is generated according to the principle of ECR. This ECR plasma is transported along some magnetic field lines (9) of the diverging inhomogeneous magnetic field in the reaction chamber (5) and introduced into the reaction chamber (5). In the reaction chamber (5), the magnetic field lines (9) are scanned by magnetic coils (two people), so the incident angle of the incident ECR plasma with respect to it changes continuously depending on the position of the sample (8) surface. The sample (8) surface is reached and etching progresses. As a result, as shown in FIG. 3, a thin film to be processed (8b) having a nearly vertical etched shape is obtained.

なお、第2図の他の実施例に示したじゃへい板(10)
を設けることにより更に垂直成分の多いプラズマを試料
(8)表面に到達させることができる。
In addition, the jacket plate (10) shown in the other embodiment in FIG.
By providing this, plasma with more vertical components can reach the surface of the sample (8).

また、上述した実施例では、反応室(5)内の磁力線(
9)を走査するために、反応室(5)内部に他の磁気コ
イル(2人)を設けたが、これを反応室(5)外に設け
ても同様の効果が得られる。更に、磁気コイル(2A)
は1個でなく、複数個設けても同様の効果が得られる。
In addition, in the above-mentioned embodiment, the magnetic field lines (
9), other magnetic coils (two persons) were provided inside the reaction chamber (5), but the same effect can be obtained even if these are provided outside the reaction chamber (5). Furthermore, magnetic coil (2A)
The same effect can be obtained by providing not only one but a plurality of them.

更に、プラズマの生成はECR放電によりなされたが、
この発明はこれに限定されることなく、高周波放電、マ
グネトロン放電、PIB放電などの他の放電形式であっ
ても上記実施例と同様の効果を得ることができる。
Furthermore, the plasma was generated by ECR discharge,
The present invention is not limited thereto, and the same effects as in the above embodiments can be obtained even with other discharge types such as high frequency discharge, magnetron discharge, and PIB discharge.

[発明の効果] この発明は、以上説明したとおり、プラズマ発生室の周
囲に設けられた磁気コイルが発生する不均一磁界の磁力
線を走査する他の磁気コイルを反応室の内部または外部
に設けたことにより、試料表面に入射衝突するプラズマ
の角度を可変にでき、従ってエツチング形状の非対称性
を解消し、加工形状の垂直性および面内均一性を向上さ
せ得る効果を奏す。
[Effects of the Invention] As explained above, the present invention provides a method in which another magnetic coil is provided inside or outside the reaction chamber to scan the lines of magnetic force of the non-uniform magnetic field generated by the magnetic coil provided around the plasma generation chamber. This makes it possible to vary the angle of the plasma that impinges on the sample surface, thereby eliminating the asymmetry of the etched shape and improving the perpendicularity and in-plane uniformity of the processed shape.

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

第1図はこの発明の一実施例を示す断面図、第2図は他
の実施例を示す断面図、そして第3図はこの発明のプラ
ズマ反応装置によって得られた試料の加工形状を示す拡
大断面図、第4図は従来のプラズマ反応装置を示す断面
図、第5図は従来のプラズマ反応装置によって得られた
試料の加工形状を示す拡大断面図である。 図において、(1)はプラズマ発生室、(2)は磁気コ
イル、(2人)は他の磁気コイル、(5)は反応室、(
8)は試料、(9)は磁力線である。 なお、各図中同一符号は同一または相当部分を示す。 児1図 蔦2図
Fig. 1 is a cross-sectional view showing one embodiment of the present invention, Fig. 2 is a cross-sectional view showing another embodiment, and Fig. 3 is an enlarged view showing the processed shape of a sample obtained by the plasma reactor of the present invention. 4 is a sectional view showing a conventional plasma reactor, and FIG. 5 is an enlarged sectional view showing the processed shape of a sample obtained by the conventional plasma reactor. In the figure, (1) is a plasma generation chamber, (2) is a magnetic coil, (2 people) is another magnetic coil, (5) is a reaction chamber, (
8) is the sample, and (9) is the magnetic field line. Note that the same reference numerals in each figure indicate the same or corresponding parts. Child 1 figure Ivy 2 figure

Claims (1)

【特許請求の範囲】 プラズマを発生するプラズマ発生室と、このプラズマを
発生室と連通しており、前記プラズマに試 よつて処理される試料を収容する反応室と、前記プラズ
マ発生室の周囲に設けられ、前記プラズマ発生室に導入
されたマイクロ波と相互作用して前記プラズマを発生さ
せる不均一磁界を発生する磁気コイルとを備えたプラズ
マ反応装置において、前記不均一磁界の磁力線を走査す
る他の磁気コイルを前記反応室の内部または外部に設け
たことを特徴とするプラズマ反応装置。
[Scope of Claims] A plasma generation chamber that generates plasma, a reaction chamber that communicates the plasma with the generation chamber and accommodates a sample to be treated by the plasma, and a reaction chamber that communicates the plasma with the generation chamber, and that surrounds the plasma generation chamber. A plasma reactor comprising: a magnetic coil configured to generate a non-uniform magnetic field that interacts with microwaves introduced into the plasma generation chamber to generate the plasma; A plasma reaction apparatus characterized in that a magnetic coil is provided inside or outside the reaction chamber.
JP63292419A 1988-11-21 1988-11-21 Plasma reaction device Pending JPH02139924A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63292419A JPH02139924A (en) 1988-11-21 1988-11-21 Plasma reaction device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63292419A JPH02139924A (en) 1988-11-21 1988-11-21 Plasma reaction device

Publications (1)

Publication Number Publication Date
JPH02139924A true JPH02139924A (en) 1990-05-29

Family

ID=17781544

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63292419A Pending JPH02139924A (en) 1988-11-21 1988-11-21 Plasma reaction device

Country Status (1)

Country Link
JP (1) JPH02139924A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04306598A (en) * 1990-10-16 1992-10-29 Internatl Business Mach Corp <Ibm> Method for generating flow of ion to electronic cyclotron resonance apparatus and substrate
JPH07201494A (en) * 1994-12-24 1995-08-04 Sony Corp Ecr plasma generator
JP2013216949A (en) * 2012-04-10 2013-10-24 Kojima Press Industry Co Ltd Plasma cvd apparatus

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04306598A (en) * 1990-10-16 1992-10-29 Internatl Business Mach Corp <Ibm> Method for generating flow of ion to electronic cyclotron resonance apparatus and substrate
JPH07201494A (en) * 1994-12-24 1995-08-04 Sony Corp Ecr plasma generator
JP2013216949A (en) * 2012-04-10 2013-10-24 Kojima Press Industry Co Ltd Plasma cvd apparatus

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