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JPH064917B2 - Plasma processing device - Google Patents
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JPH064917B2 - Plasma processing device - Google Patents

Plasma processing device

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Publication number
JPH064917B2
JPH064917B2 JP7394189A JP7394189A JPH064917B2 JP H064917 B2 JPH064917 B2 JP H064917B2 JP 7394189 A JP7394189 A JP 7394189A JP 7394189 A JP7394189 A JP 7394189A JP H064917 B2 JPH064917 B2 JP H064917B2
Authority
JP
Japan
Prior art keywords
coil
sample
magnetic field
plasma
distribution
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
JP7394189A
Other languages
Japanese (ja)
Other versions
JPH02254170A (en
Inventor
幹保 木内
誠太郎 松尾
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.)
NTT Inc
Original Assignee
Nippon Telegraph and Telephone 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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP7394189A priority Critical patent/JPH064917B2/en
Publication of JPH02254170A publication Critical patent/JPH02254170A/en
Publication of JPH064917B2 publication Critical patent/JPH064917B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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] 本発明はプラズマおよびそれに含まれるイオンを利用し
て材料表面上に薄膜を形成するために、または材料表面
をエッチングするために用いるプラズマ処理装置に関す
るものであり、特に半導体集積回路などの各種デバイス
の製造工程に適合するプラズマ処理装置に関するもので
ある。
The present invention relates to a plasma processing apparatus used for forming a thin film on a material surface using plasma and ions contained therein, or for etching the material surface. In particular, the present invention relates to a plasma processing apparatus suitable for manufacturing processes of various devices such as semiconductor integrated circuits.

[従来の技術] 薄膜形成およびエッチングに用いるプラズマ生成法とし
て、マイクロ波励起による電子サイクロトロン共鳴を利
用したプラズマ生成法があり、これは低ガス圧,高イオ
ン化率,高活性の特徴を有し、導入ガスの選択,イオン
エネルギーの制御によって優れた加工特性を発揮しうる
ことが明らかにされている。
[Prior Art] As a plasma generation method used for thin film formation and etching, there is a plasma generation method using electron cyclotron resonance by microwave excitation, which has features of low gas pressure, high ionization rate, and high activity, It has been clarified that excellent processing characteristics can be achieved by selecting the introduced gas and controlling the ion energy.

第7図にマイクロ波電子サイクロトロン共鳴プラズマを
利用した、従来のプラズマ処理装置の基本構成図を示
す。ここに、1は、プラズマ生成室、2は試料室、12は
排気路、3はマイクロ波導入窓であって例えば石英ガラ
ス板により構成されている。4はマイクロ波導入のため
の矩形導波管である。9はプラズマ生成室1で生成され
たプラズマを試料台10載置された試料11に導くためのプ
ラズマ引出し窓である。13はプラズマ生成室1の内部の
適当な領域で電子サイクロトロン共鳴条件を満す磁界強
度を発生させるための磁気コイルであり、プラズマ流8
を形成させるための発散磁界の形成にも利用している。
図示を省略したマイクロ波源は、例えば周波数2.45GHZ
のマグネトロンを用いて構成される。5はプラズマ生成
室の冷却水路、6および7はガス導入用の第1ガス導入
系および第2ガス導入系であり、処理目的に応じて、そ
れぞれ単独もしくは組合せて使用する。
FIG. 7 shows a basic configuration diagram of a conventional plasma processing apparatus using microwave electron cyclotron resonance plasma. Here, 1 is a plasma generation chamber, 2 is a sample chamber, 12 is an exhaust passage, and 3 is a microwave introduction window, which is made of, for example, a quartz glass plate. Reference numeral 4 is a rectangular waveguide for introducing microwaves. Reference numeral 9 is a plasma extraction window for guiding the plasma generated in the plasma generation chamber 1 to the sample 11 mounted on the sample table 10. Reference numeral 13 is a magnetic coil for generating a magnetic field strength satisfying the electron cyclotron resonance condition in an appropriate region inside the plasma generation chamber 1, and the plasma flow 8
It is also used to form a divergent magnetic field to form
Microwave source, not shown, for example a frequency 2.45 GHz Z
Composed of a magnetron. Reference numeral 5 is a cooling water passage of the plasma generation chamber, and 6 and 7 are a first gas introduction system and a second gas introduction system for introducing gas, which are used alone or in combination depending on the processing purpose.

例えば、窒化シリコン膜の形成には第1ガス導入系6よ
りガスを導入し、第2ガス導入系7からSiH4ガスを導入
する。エッチングの場合は第1ガス導入系6または第2
ガス導入系7からcl2,SF6,02などのエッチング用ガスを
導入する。
For example, in forming the silicon nitride film, gas is introduced from the first gas introduction system 6 and SiH 4 gas is introduced from the second gas introduction system 7. In the case of etching, the first gas introduction system 6 or the second
Introducing an etching gas from the gas introduction system 7 such as cl 2, SF 6, 0 2 .

このような、薄膜形成やエッチングでの処理加工の試料
面内分布は、プラズマ生成室1で生成されるプラズマ密
度、引出されるプラズマ流の密度などに依存してある程
度の不均一性を持っているため、大面積の試料に適用す
るには、さらに均一性を向上させる必要がある。薄膜の
形成やエッチングの反応は、主に発散磁界の磁力線に沿
ってサイクロトロン運動した電子と、電子とガス分子と
の衝突により発生したイオンにより促進されることか
ら、発散磁界分布を制御することでプラズマ処理速度の
試料面内分布を改善することが考えられる。
The in-plane distribution of the sample in the thin film formation and the processing by etching has a certain degree of non-uniformity depending on the density of the plasma generated in the plasma generation chamber 1 and the density of the drawn plasma flow. Therefore, it is necessary to further improve the uniformity in order to apply it to a large area sample. The reaction of thin film formation and etching is mainly promoted by the electrons that have undergone cyclotron motion along the magnetic field lines of the divergent magnetic field and the ions generated by the collision of the electrons with the gas molecules. It is considered to improve the in-plane distribution of the plasma processing rate of the sample.

第8図に、従来の磁界分布補正用コイルを付加したプラ
ズマ処理装置の概略構成図を示す。この図は試料室を拡
大して示しており、他の部分の構成は第7図と同様であ
る。試料台10の裏側にソレノイドコイル14を配置し、発
散磁界用の磁気コイル13に対して逆方向電流を流すこと
により、試料面内の発散磁界分布を制御するものであ
る。
FIG. 8 shows a schematic configuration diagram of a plasma processing apparatus to which a conventional magnetic field distribution correction coil is added. This drawing shows an enlarged view of the sample chamber, and the configuration of the other parts is the same as in FIG. A solenoid coil 14 is arranged on the back side of the sample table 10 and a reverse current is applied to the magnetic coil 13 for divergent magnetic field to control the divergent magnetic field distribution in the sample surface.

[発明が解決しようとする課題] 第8図の構成により均一性を改善することはある程度可
能であるが、コイルがソレノイド状であるため、発散磁
界分布の制御が部分的になり、平坦な処理速度分布が得
られにくいこと、コイルの容積が大きくなるため試料台
とは別に設置場所を確保する必要があること、しかもコ
イルからの吸着ガス、ゴミの発生を防止するため、コイ
ルを試料室の外に設置することなど、装置構成上いろい
ろ制限される問題が生じる。試料面内の磁界分布を最適
な分布に広範囲に制御でき、しかも小型で薄いコイルが
できれば、さらに処理面積の拡大、処理速度の向上など
大幅な特性向上が期待できるとともに装置構成が容易に
なる。
[Problems to be Solved by the Invention] Although it is possible to improve the uniformity to some extent by the configuration of FIG. 8, since the coil has a solenoidal shape, the divergent magnetic field distribution is partially controlled and a flat process is performed. It is difficult to obtain a velocity distribution, the volume of the coil becomes large, and it is necessary to secure an installation place separately from the sample table.Moreover, in order to prevent the generation of adsorbed gas and dust from the coil, keep the coil in the sample chamber. There are various restrictions on the device configuration such as installation outside. If the magnetic field distribution in the sample surface can be controlled over a wide range to the optimum distribution, and if a small and thin coil can be made, it is possible to expect a significant improvement in characteristics such as an increase in processing area and an increase in processing speed, and the device configuration will be easy.

本発明は上述した従来の欠点を解決し、プラズマ流の発
散磁界分布を広範囲に制御し、処理速度の均一性を向上
させ、処理面積や処理速度を向上させうるプラズマ処理
装置を提供することを目的とする。
The present invention solves the above-mentioned conventional drawbacks, provides a plasma processing apparatus capable of controlling the divergent magnetic field distribution of a plasma flow over a wide range, improving the uniformity of the processing speed, and improving the processing area and the processing speed. To aim.

[課題を解決するための手段] 本発明はマイクロ波を利用してプラズマを生成し、プラ
ズマまたはプラズマ中の主としてイオンを試料に照射し
て処理を行うプラズマ処理装置において、試料を保持す
るための試料台の試料保持面と反対側の面に、試料台表
面近傍の磁界分布を制御するための少なくとも1個の偏
平コイルを具えたことを特徴とする。
[Means for Solving the Problems] The present invention is directed to holding a sample in a plasma processing apparatus that generates plasma using microwaves and irradiates the sample with plasma or mainly ions in the plasma to perform processing. At least one flat coil for controlling the magnetic field distribution near the surface of the sample table is provided on the surface of the sample table opposite to the sample holding surface.

[作用] 本発明の偏平コイルは直径方向に渦巻き状に巻いた薄い
円板状のコイルであり、プラズマ生成室から引き出され
る発散磁界の試料台表面近傍の磁界分布を、コイルの巻
線密度分布、試料台とコイルとの距離、およびコイル電
流を設定することにより広範囲に制御し、均一性のよい
平坦なプラズマ処理速度を可能にする。コイルと試料台
との組合わせはコイル全体の厚さが薄いため、試料台と
一体に構成することが可能であり、また、試料を冷却す
るために、冷却水を試料台に循環する構造にすれば、コ
イルの冷却との併用もでき有効である。さらに、試料台
に試料を保持するための静電吸着方式および試料にバイ
アスを付加する。RF印加方式を採用した場合も、試料台
に本発明の偏平コイルを組込むことが可能である。
[Operation] The flat coil of the present invention is a thin disk-shaped coil wound spirally in the diametrical direction. By controlling the distance between the sample stage and the coil, and the coil current, a wide range of control is possible, and a flat plasma processing rate with good uniformity is possible. The combination of the coil and the sample stage can be configured integrally with the sample stage because the entire coil is thin, and the cooling water is circulated to the sample stage to cool the sample. If so, it can be used together with cooling of the coil, which is effective. Further, a bias is applied to the electrostatic attraction method for holding the sample on the sample table and the sample. Even when the RF application method is adopted, the flat coil of the present invention can be incorporated in the sample table.

[実施例] 以下に図面を参照して本発明の実施例を説明する。Embodiments Embodiments of the present invention will be described below with reference to the drawings.

第1図に本発明を実施したプラズマ処理装置の構成を示
す。第1図は試料室を拡大して示しており、他の部分の
構成は、第7図と同様である。プラズマ生成室1のプラ
ズマ引出し窓9を通って導かれたプラズマ流8により、
試料台10上の試料11をプラズマ処理する。その試料台10
の裏面に偏平コイル15を発散磁界発生用の磁気コイル13
と中心軸を一致させて配置した。偏平コイルは中心軸部
から直径方向に渦巻状に巻いた構造で、実験例ではコイ
ル線として線径1.5mmのポリイミド被覆銅線を用い、磁
界強度を増すため、2枚重ねにしてあり、コイル全体の
厚さは約3mm、直径は10〜20cm程度である。
FIG. 1 shows the configuration of a plasma processing apparatus embodying the present invention. FIG. 1 shows the sample chamber in an enlarged scale, and the configuration of the other parts is the same as in FIG. By the plasma flow 8 guided through the plasma extraction window 9 of the plasma generation chamber 1,
A sample 11 on the sample table 10 is plasma-processed. The sample table 10
A flat coil 15 is placed on the back side of the magnetic coil 13 for generating a divergent magnetic field.
And the central axes are aligned. The flat coil has a structure in which it is spirally wound in the diameter direction from the central axis. In the experimental example, a polyimide-coated copper wire with a wire diameter of 1.5 mm was used as the coil wire, and two layers were stacked to increase the magnetic field strength. The total thickness is about 3 mm and the diameter is about 10 to 20 cm.

このような構成によって、発散磁界で引出されたプラズ
マ流の試料面内の磁界分布を、発散磁界と逆方向の磁界
を発生させる偏平コイルにより制御する。発散磁界のみ
の試料面内の磁界強度は中央部が高く(115G)円周部に
なるほどゆるやかに低下した(中心より9cm離れた位置
で100G)分布を持っている。
With such a configuration, the magnetic field distribution in the sample surface of the plasma flow extracted by the divergent magnetic field is controlled by the flat coil that generates a magnetic field in the direction opposite to the divergent magnetic field. The magnetic field strength in the plane of the sample with only the divergent magnetic field is high in the central part (115 G) and gradually decreases toward the circumferential part (100 G at a position 9 cm away from the center).

本発明の偏平コイルを用いた効果を確認するため、酸化
シリコン膜について膜形成実験を行なった。膜形成条件
はこの実験では、O2:30cc/min,SiH4:30cc/min,マイクロ
波パワー:200Wとした。試料は5インチないし6インチ
のSiウェーハを使用した。
In order to confirm the effect of using the flat coil of the present invention, a film formation experiment was conducted on a silicon oxide film. In this experiment, the film forming conditions were O 2 : 30 cc / min, SiH 4 : 30 cc / min, and microwave power: 200 W. As the sample, a 5 inch to 6 inch Si wafer was used.

第2図に円板状の偏平コイルの概略構成図を示す。コイ
ルは中心軸から直径方向へ渦巻状に順次巻いた巻線密度
の高いもので直径14cmであり、コイルと試料は5mm離し
た。第3図にこの円板状の偏平コイルを用いた場合の磁
界分布と膜形成速度分布を示す。このコイルの磁界分布
は、コイル中央が最も磁界が強いピラミッド状である。
得られた膜形成速度分布はコイルを使用しない場合に比
べて、コイル電流5Aで中心部4cmの範囲が平坦になり、
さらにコイル電流7.5Aでは、中心部7cmの範囲が平坦に
なった。
FIG. 2 shows a schematic configuration diagram of a disk-shaped flat coil. The coil had a high winding density, which was wound in a spiral shape from the central axis in the direction of diameter, and had a diameter of 14 cm. The coil and the sample were separated by 5 mm. FIG. 3 shows the magnetic field distribution and the film formation speed distribution when this disk-shaped flat coil is used. The magnetic field distribution of this coil has a pyramid shape in which the magnetic field is strongest at the center of the coil.
The obtained film formation rate distribution is flatter in the central area of 4 cm at a coil current of 5 A, as compared with the case where no coil is used.
Furthermore, at a coil current of 7.5 A, the central area of 7 cm became flat.

第4図に、ドーナツ状の偏平コイルの概略構成図を示
す。コイル形状は、直径18cmで中心部の直径10cmを中空
にしたもので、このコイルと試料台との距離は多少なだ
らかな磁界分布とするため10mmとした。第5図にこのド
ーナツ状の偏平コイルを用いた場合のその磁界分布と膜
形成速度分布を示す。このコイルの磁界分布は、ほぼ台
形状となっており、この台形の上辺に相当した部分がコ
イルの中空径10cmに対応したかたちとなっている。実際
の試料面内分布は発散磁界分布との合成になり、直径10
cmの外周部分が高い磁界強度となる。このコイルを使用
した結果、膜形成速度分布は広範囲にわたって、均一性
の改善が認められ、たとえば試料面の中心と±6.5cmの
位置とではコイルを使用しないと±10%の不均一性があ
るのに対し、コイル電流10Aでは±5%と、従来の半分
に不均一性を低減できた。第6図は、巻線密度を考えた
場合の偏平コイルの概略構成図を示す。コイル中央部は
ある程度間隔をとって巻き、周辺部はつめて巻いた構造
で、このコイルの磁界分布はコイル中央部から円周部に
ゆるやかに低下した曲線状をとるため、発散磁界の制御
性が一段と高まり、さらに試料面内分布の均一性の向上
が図れる。
FIG. 4 shows a schematic configuration diagram of a donut-shaped flat coil. The coil shape is 18 cm in diameter and 10 cm in the center is made hollow, and the distance between this coil and the sample stage is set to 10 mm in order to have a somewhat gentle magnetic field distribution. FIG. 5 shows the magnetic field distribution and film formation speed distribution when this donut-shaped flat coil is used. The magnetic field distribution of this coil is almost trapezoidal, and the part corresponding to the upper side of this trapezoid corresponds to the coil hollow diameter of 10 cm. The actual sample in-plane distribution is a composite with the divergent magnetic field distribution, and the diameter of 10
The magnetic field strength is high at the outer periphery of cm. As a result of using this coil, the uniformity of the film formation rate distribution was found to be improved over a wide range, and for example, there is ± 10% non-uniformity between the center of the sample surface and the position of ± 6.5 cm unless the coil is used. On the other hand, with a coil current of 10 A, the nonuniformity was reduced to ± 5%, which is half that of the conventional method. FIG. 6 shows a schematic configuration diagram of a flat coil in consideration of winding density. The central part of the coil is wound with a certain interval, and the peripheral part is wound tightly.The magnetic field distribution of this coil has a gently-decreasing curved shape from the central part of the coil to the circumferential part. Is further increased, and the uniformity of the in-plane distribution of the sample can be improved.

なお、本発明の変形として、磁界分布を設定した板状永
久磁石の利用や、本発明と軟鉄などの高透磁率材料との
組合せによって、同様の効果をもたらす磁界分布を形成
することもできる。また、複数個の偏平コイルを組合わ
せて、磁界分布の制御性をさらに高めることも可能であ
る。
As a modification of the present invention, it is possible to form a magnetic field distribution that brings about the same effect by using a plate-shaped permanent magnet having a set magnetic field distribution or by combining the present invention with a high magnetic permeability material such as soft iron. Further, it is possible to further enhance the controllability of the magnetic field distribution by combining a plurality of flat coils.

[発明の効果] 以上の説明から明らかなように、本発明の装置において
は偏平コイルを用いて発散磁界の分布を広範囲に制御で
きるようにしたので、プラズマ処理速度の均一性が向上
し、プラズマ処理面積の広大、スループットの向上を実
現できるとともに、装置構成上は、試料台との組合わせ
が容易になる利点がある。
[Effects of the Invention] As is clear from the above description, in the apparatus of the present invention, the flat coil is used to control the distribution of the divergent magnetic field over a wide range, so that the uniformity of the plasma processing rate is improved and There is an advantage that the processing area can be widened and the throughput can be improved, and in terms of the apparatus configuration, it can be easily combined with the sample table.

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

第1図は本発明の実施例の概要図、第2図は円板状偏平
コイルの概略断面図、第3図は円板状偏平コイルを用い
た場合の磁界分布とSiO2膜形成速度分布を示す図、第4
図はドーナツ状偏平コイルの概略断面図、第5図はドー
ナツ状偏平コイルを用いた場合の磁界分布とSiO2膜形成
速度分布を示す図、第6図は巻線密度を変えた偏平コイ
ルの概略断面図、第7図はプラズマ処理装置の基本構成
図、第8図は従来の磁界分布補正用コイルを用いた装置
の概要図である。 1…プラズマ生成室、2…試料室、3…マイクロ波導入
窓、4…矩形導波管、5…冷却水路、6…第1ガス導入
系、7…第2ガス導入系、8…プラズマ流、9…プラズ
マ引出し窓、10…試料台、11…試料、12…排気系、13…
磁気コイル、14…ソレノイドコイル、15…偏平コイル。
FIG. 1 is a schematic diagram of an embodiment of the present invention, FIG. 2 is a schematic sectional view of a disk-shaped flat coil, and FIG. 3 is a magnetic field distribution and a SiO 2 film formation rate distribution when the disk-shaped flat coil is used. Showing the fourth
The figure is a schematic cross-sectional view of a donut-shaped flat coil. Fig. 5 shows the magnetic field distribution and SiO 2 film formation rate distribution when the donut-shaped flat coil is used. Fig. 6 shows the flat coil with different winding density. FIG. 7 is a schematic sectional view, FIG. 7 is a basic configuration diagram of a plasma processing apparatus, and FIG. 8 is a schematic view of an apparatus using a conventional magnetic field distribution correction coil. 1 ... Plasma generation chamber, 2 ... Sample chamber, 3 ... Microwave introduction window, 4 ... Rectangular waveguide, 5 ... Cooling water channel, 6 ... First gas introduction system, 7 ... Second gas introduction system, 8 ... Plasma flow , 9 ... Plasma extraction window, 10 ... Sample stage, 11 ... Sample, 12 ... Exhaust system, 13 ...
Magnetic coil, 14 ... Solenoid coil, 15 ... Flat coil.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】マイクロ波を利用してプラズマを生成し、
該プラズマまたは該プラズマ中の主としてイオンを試料
に照射して処理を行うプラズマ処理装置において、前記
試料を保持するための試料台の試料保持面と反対側の面
に、試料台表面近傍の磁界分布を制御するための少なく
とも1個の偏平コイルを具えたことを特徴とするプラズ
マ処理装置。
1. A plasma is generated using microwaves,
In a plasma processing apparatus that performs processing by irradiating a sample with the plasma or mainly ions in the plasma, a magnetic field distribution near the surface of the sample table on a surface of the sample table opposite to the sample holding surface for holding the sample. A plasma processing apparatus, comprising at least one flat coil for controlling the temperature.
JP7394189A 1989-03-28 1989-03-28 Plasma processing device Expired - Lifetime JPH064917B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7394189A JPH064917B2 (en) 1989-03-28 1989-03-28 Plasma processing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7394189A JPH064917B2 (en) 1989-03-28 1989-03-28 Plasma processing device

Publications (2)

Publication Number Publication Date
JPH02254170A JPH02254170A (en) 1990-10-12
JPH064917B2 true JPH064917B2 (en) 1994-01-19

Family

ID=13532639

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7394189A Expired - Lifetime JPH064917B2 (en) 1989-03-28 1989-03-28 Plasma processing device

Country Status (1)

Country Link
JP (1) JPH064917B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2840700B2 (en) * 1990-12-31 1998-12-24 株式会社 半導体エネルギー研究所 Film forming apparatus and film forming method

Also Published As

Publication number Publication date
JPH02254170A (en) 1990-10-12

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