JPS5927213B2 - plasma reactor - Google Patents
plasma reactorInfo
- Publication number
- JPS5927213B2 JPS5927213B2 JP54125091A JP12509179A JPS5927213B2 JP S5927213 B2 JPS5927213 B2 JP S5927213B2 JP 54125091 A JP54125091 A JP 54125091A JP 12509179 A JP12509179 A JP 12509179A JP S5927213 B2 JPS5927213 B2 JP S5927213B2
- Authority
- JP
- Japan
- Prior art keywords
- plasma
- electrodes
- etching
- magnetic field
- gas
- 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
Links
Landscapes
- ing And Chemical Polishing (AREA)
- Drying Of Semiconductors (AREA)
- Plasma Technology (AREA)
- Physical Or Chemical Processes And Apparatus (AREA)
Description
【発明の詳細な説明】
この発明は、平行平板型プラズマエッチング及ひプラズ
マCVl)成膜装置のエッチング特性及ひ成膜特性の改
良に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in the etching characteristics and film forming characteristics of a parallel plate type plasma etching and plasma CVl) film forming apparatus.
従来の平行平板型プラズマエッチング及ひプラズマCV
D成膜装置の概略図を第1図に示す。Conventional parallel plate plasma etching and plasma CV
A schematic diagram of the D film forming apparatus is shown in FIG.
従来の装置においては、全極性高周波電極1及び2が真
空槽3の中に対向電極構造的に配置され、例えば第1図
に示されたごとく、高周波電源4からの高周波電力を金
属性高周波電極1及び2の間に印加し、ガスプラズマ6
を電極1及び2の間に発生させる。プラズマの発生条件
は電極1及び2の間隔、電極間のガス圧力、印加高周波
の周波数で決める。この条件は、高周波放電に対するパ
ツシエンの法則として知られている。さて、この様な平
行平板型プラズマ発生装置を用いて、例えばいわゆるプ
ラズマエッチングを行う場合、エッチングされる材料5
、例えば、シリコン基板やこのシリコン基板上に形成さ
れたシリコン化合物等は、第1図の如く、対向電極の一
方の表面に置かれる。例えば、半導体装置の作成に広<
利用される酸化シリコンやリンやヒ素を含んた酸化シリ
コン膜などをこの装置によつてエッチングする場合、ガ
スとしてC9F8ガスやCHF3ガス、CF4+H2ガ
スなどが用いられる。エッチングを安定に行うためには
、対向電極1と2の間のプラズマ6が安定に形成され、
しかもエッチングされる材料5の表面近傍Tのプラズマ
状態を安定化する必要がある。この表面近傍1のプラズ
マ状態は、対向電極1、2間のガスの流れ方、つまυ濃
度分布、特に、エッチングされる材料5の表面近傍のガ
スの濃度分布と流速分布に入きく依存する。通常、第1
図の如き装置においては、プラズマ状態を安定に保つこ
とは難しい。例えば、エッチングを行う毎にエッチング
特性が変化するといつた不安定性が第1図の如き構造の
場合にはどうしてもさけられない。この発明の目的は、
対向電極1、2の一部あるいは全面に磁場発生部材をう
め込み、電極1、2間のプラズマ状態を磁場印加効果に
より安定させようとするものである。以下、この発明の
詳細な内容を第2図の実施例に従つて説明する。In the conventional device, all-polar high-frequency electrodes 1 and 2 are arranged in a vacuum chamber 3 in a counter-electrode structure, and, as shown in FIG. 1 and 2, gas plasma 6
is generated between electrodes 1 and 2. The plasma generation conditions are determined by the distance between electrodes 1 and 2, the gas pressure between the electrodes, and the frequency of the applied high frequency. This condition is known as Patsien's law for high frequency discharges. Now, when performing so-called plasma etching using such a parallel plate type plasma generator, for example, the material to be etched 5
For example, a silicon substrate or a silicon compound formed on the silicon substrate is placed on one surface of the counter electrode, as shown in FIG. For example, it is widely used in the production of semiconductor devices.
When etching a silicon oxide film or a silicon oxide film containing phosphorus or arsenic to be used, the gas used is C9F8 gas, CHF3 gas, CF4+H2 gas, or the like. In order to perform etching stably, the plasma 6 between the opposing electrodes 1 and 2 must be stably formed,
Moreover, it is necessary to stabilize the plasma state near the surface T of the material 5 to be etched. The plasma state near the surface 1 depends on the way the gas flows between the opposing electrodes 1 and 2, the concentration distribution of the gas, and especially the concentration distribution and flow velocity distribution of the gas near the surface of the material 5 to be etched. Usually the first
In the apparatus shown in the figure, it is difficult to maintain a stable plasma state. For example, instabilities such as changes in etching characteristics each time etching is unavoidable in the structure shown in FIG. 1. The purpose of this invention is to
A magnetic field generating member is embedded in a part or the entire surface of the opposing electrodes 1 and 2, and the plasma state between the electrodes 1 and 2 is stabilized by the effect of applying a magnetic field. The detailed contents of this invention will be explained below according to the embodiment shown in FIG.
第2図に示した実施例は、金属製対向電極1、2、真空
槽3、高周波電源4、及び対向電極1,2にうめ込まれ
た磁石9から構成される。この実施例では、エツチング
される材料5の位置に対応した電極1,2内に永久磁石
がうめ込まれている。次に、この実施例の動作、効果に
ついて説明する。第1図の場合と同様に、対向電極1,
2の置かれた真空槽3内を排気系8を動作させて、所定
の圧力まで排気した後、真空槽3内に、エツチングされ
る材料5に合致したガス、例えば、酸化シリコン膜の場
合にはC3F8ガスを導入し、真空槽3内のガス圧を所
定の値、例えば0.1t0rrに保つ。次に、高周波電
源4を動作させて、対向電極1,2の間に、所定の周波
数の高周波電力(例えば13MHzで1KW)を印加し
、対向電極1,2間にプラズマを発生させる。第2図の
場合、電極1、あるいは電極1と2の両方に、予めうめ
込まれた磁石9により、対向電極1,2の表面と垂直方
向に靜磁場10が存在する。この静磁場は、対応電極1
と2の間に高周波放電を発生させる場合に、相対的に放
電開始電圧を低くする効果があるために、従来の第1図
の場合に比ベプラズマ発生を容易にし、しかもプラズマ
が発生した後に、プラズマ状態の安定な維持に寄与する
プラズマ中の電子やイオンの運動方向を磁力線で制御す
るため、安定なプラズマ状態を対向電極1と2の間に形
成する役目を果たす。第3図に、第1図従来装置とこの
発明の第2図実施例とを比較して、プラズマの安定性と
プラズマ維持時間を示した。第2図(破線で示す)の場
合は、第1図(実線で示す)に比べ、明らかにプラズマ
の安定度が良く、しかも、安定状態に達する迄の時間が
著しく短いことが確認された。さらに、この第2図実施
例を、例えば酸化シリコン膜のエツチングに用いる事に
より、基板5内のエツチング量の均一性も著しく向上し
た。例えば、同一ブラズマ条件下では均一性は約3倍改
良された。上記の説明により、対向電極1,2に磁場発
生用磁石9をうめ込む事により対向電極1,2間のプラ
ズマを安定化出来ることが示された。The embodiment shown in FIG. 2 is composed of metal counter electrodes 1, 2, a vacuum chamber 3, a high frequency power source 4, and a magnet 9 embedded in the counter electrodes 1, 2. In this embodiment, permanent magnets are embedded in the electrodes 1, 2 corresponding to the location of the material 5 to be etched. Next, the operation and effects of this embodiment will be explained. As in the case of FIG. 1, the counter electrode 1,
After operating the exhaust system 8 to evacuate the inside of the vacuum chamber 3 in which the etching material 2 is placed to a predetermined pressure, a gas matching the material 5 to be etched, for example, in the case of a silicon oxide film, is added to the vacuum chamber 3. C3F8 gas is introduced, and the gas pressure in the vacuum chamber 3 is maintained at a predetermined value, for example, 0.1 t0rr. Next, the high frequency power source 4 is operated to apply high frequency power at a predetermined frequency (for example, 1 KW at 13 MHz) between the opposing electrodes 1 and 2 to generate plasma between the opposing electrodes 1 and 2. In the case of FIG. 2, a static magnetic field 10 exists in the direction perpendicular to the surfaces of the opposing electrodes 1 and 2 due to the magnet 9 embedded in the electrode 1 or both electrodes 1 and 2 in advance. This static magnetic field is applied to the corresponding electrode 1
When a high-frequency discharge is generated between Since the direction of movement of electrons and ions in the plasma, which contribute to maintaining a stable plasma state, is controlled by magnetic lines of force, it serves to form a stable plasma state between the opposing electrodes 1 and 2. FIG. 3 shows the plasma stability and plasma maintenance time by comparing the conventional device shown in FIG. 1 with the embodiment shown in FIG. 2 of the present invention. In the case of FIG. 2 (indicated by a broken line), it was confirmed that the stability of the plasma was clearly better than in FIG. 1 (indicated by a solid line), and the time required to reach a stable state was significantly shorter. Furthermore, by using the embodiment shown in FIG. 2 for etching a silicon oxide film, for example, the uniformity of the etching amount within the substrate 5 was significantly improved. For example, uniformity was improved by about 3 times under the same plasma conditions. The above explanation shows that the plasma between the opposing electrodes 1 and 2 can be stabilized by embedding the magnetic field generating magnet 9 in the opposing electrodes 1 and 2.
ブラズマ状態、特にエツチングされる材料5の表面近傍
のプラズマ状態がエツチング特性に影響する。したがつ
て、他の実施例として、うめ込み永久磁石9の代りに、
対向電極1,2内に電磁石を構成するための磁場発生用
コイル11をうめ込んだ例を第4図に示す。この場合に
は、うめこんだコイル11に外部から直流電流を印加し
、対向電極1,2の間に静磁場を発生させるが、この静
磁場の強度はコイル11に流す直流電流の値により自由
に変化出来る。したがつて、このコイル11に流す直流
電流により、対向電極1,2間及びエツチングされる材
料5の表面近傍のプラズマ状態を大巾に変化させること
が出来、エツチング特性を外部から任意に制御出来る。
な卦この発明の装置はブラズマエツチングのみならずプ
ラズマCVD(化学的気相成長法)による成膜にも適用
出来る。The plasma state, especially the plasma state near the surface of the material 5 to be etched, influences the etching characteristics. Therefore, in another embodiment, instead of the recessed permanent magnet 9,
FIG. 4 shows an example in which a magnetic field generating coil 11 for forming an electromagnet is embedded in the opposing electrodes 1 and 2. In this case, a direct current is applied to the recessed coil 11 from the outside to generate a static magnetic field between the opposing electrodes 1 and 2, but the strength of this static magnetic field can be changed depending on the value of the direct current flowing through the coil 11. It can change to Therefore, the plasma state between the opposing electrodes 1 and 2 and near the surface of the material 5 to be etched can be greatly changed by the direct current flowing through this coil 11, and the etching characteristics can be controlled arbitrarily from the outside. .
Furthermore, the apparatus of the present invention can be applied not only to plasma etching but also to film formation by plasma CVD (chemical vapor deposition).
第1図は従来の装置の概念図、第2図はこの発明の装置
の一実施例を示す概念図、第3図はこの発明の動作説明
用線図、第4図はこの発明の他の実施例を示す概念図で
ある。
図中、1,2は高周波電極、3は真空槽、4は高周波電
源、5は材料、6はブラズマ、7は表面近傍、8は排気
系、9は永久磁石、10は静磁場、11はコイルを示す
。Fig. 1 is a conceptual diagram of a conventional device, Fig. 2 is a conceptual diagram showing an embodiment of the device of the present invention, Fig. 3 is a diagram for explaining the operation of the present invention, and Fig. 4 is a conceptual diagram of another embodiment of the device of the present invention. It is a conceptual diagram showing an example. In the figure, 1 and 2 are high frequency electrodes, 3 is a vacuum chamber, 4 is a high frequency power supply, 5 is a material, 6 is a plasma, 7 is near the surface, 8 is an exhaust system, 9 is a permanent magnet, 10 is a static magnetic field, and 11 is a The coil is shown.
Claims (1)
極の一部あるいは全面に磁場発生部材をくみ込んだこと
を特徴とするプラズマ反応装置。1. A plasma reaction device characterized in that a magnetic field generating member is embedded in a part or the entire surface of parallel plate type high frequency electrodes that are arranged oppositely in a vacuum chamber.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54125091A JPS5927213B2 (en) | 1979-09-27 | 1979-09-27 | plasma reactor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54125091A JPS5927213B2 (en) | 1979-09-27 | 1979-09-27 | plasma reactor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5648238A JPS5648238A (en) | 1981-05-01 |
| JPS5927213B2 true JPS5927213B2 (en) | 1984-07-04 |
Family
ID=14901614
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP54125091A Expired JPS5927213B2 (en) | 1979-09-27 | 1979-09-27 | plasma reactor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5927213B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5756036A (en) * | 1980-09-20 | 1982-04-03 | Mitsubishi Electric Corp | Plasma chemical vapor phase reactor |
-
1979
- 1979-09-27 JP JP54125091A patent/JPS5927213B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5648238A (en) | 1981-05-01 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5330606A (en) | Plasma source for etching | |
| US6129806A (en) | Plasma processing apparatus and plasma processing method | |
| JP2771205B2 (en) | Method and apparatus for processing solid surfaces by particle bombardment | |
| US6866753B2 (en) | Vacuum arc vapor deposition apparatus and vacuum arc vapor deposition method | |
| US6902683B1 (en) | Plasma processing apparatus and plasma processing method | |
| US20040040931A1 (en) | Plasma processing method and plasma processor | |
| US5698070A (en) | Method of etching film formed on semiconductor wafer | |
| US5345145A (en) | Method and apparatus for generating highly dense uniform plasma in a high frequency electric field | |
| US20040168771A1 (en) | Plasma reactor coil magnet | |
| US6909087B2 (en) | Method of processing a surface of a workpiece | |
| JPH04229940A (en) | Device for ion plasma mechanically processing surface of work | |
| JPS5915982B2 (en) | Electric discharge chemical reaction device | |
| US6167835B1 (en) | Two chamber plasma processing apparatus | |
| JPS6136589B2 (en) | ||
| JPS5927213B2 (en) | plasma reactor | |
| JPS5927212B2 (en) | plasma reactor | |
| JP2567892B2 (en) | Plasma processing device | |
| JPH02312231A (en) | Dryetching device | |
| JPS60163433A (en) | Plasma treatment device | |
| JPS6297329A (en) | Dry etching device | |
| GB2049560A (en) | Plasma etching | |
| JPS59139629A (en) | Plasma dry processing equipment | |
| JPS611024A (en) | Manufacturing apparatus of semiconductor circuit | |
| JPS60218826A (en) | Formation of thin film | |
| JP2956395B2 (en) | Magnetic field plasma processing equipment |