JP3920209B2 - Plasma generator - Google Patents

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Publication number
JP3920209B2
JP3920209B2 JP2002363989A JP2002363989A JP3920209B2 JP 3920209 B2 JP3920209 B2 JP 3920209B2 JP 2002363989 A JP2002363989 A JP 2002363989A JP 2002363989 A JP2002363989 A JP 2002363989A JP 3920209 B2 JP3920209 B2 JP 3920209B2
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JP
Japan
Prior art keywords
plasma
antenna
substrate
frequency
antennas
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JP2004200233A (en
Inventor
多津男 庄司
裕一 節原
明憲 江部
正司 三宅
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Japan Science and Technology Agency
National Institute of Japan Science and Technology Agency
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Japan Science and Technology Agency
National Institute of Japan Science and Technology Agency
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Priority to JP2002363989A priority Critical patent/JP3920209B2/en
Priority to TW092135000A priority patent/TW200420201A/en
Priority to TW099122628A priority patent/TWI391035B/en
Priority to TW099122626A priority patent/TW201041455A/en
Priority to CN2007101624017A priority patent/CN101128083B/en
Priority to EP10180427.6A priority patent/EP2259663B1/en
Priority to US10/539,254 priority patent/US7785441B2/en
Priority to CN2007101624036A priority patent/CN101128084B/en
Priority to EP03780748.4A priority patent/EP1575343B1/en
Priority to KR1020117019922A priority patent/KR101199994B1/en
Priority to PCT/JP2003/016007 priority patent/WO2004056159A1/en
Priority to KR1020057011022A priority patent/KR101090726B1/en
Priority to KR1020117019924A priority patent/KR101186822B1/en
Priority to KR1020117019923A priority patent/KR101199995B1/en
Publication of JP2004200233A publication Critical patent/JP2004200233A/en
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Publication of JP3920209B2 publication Critical patent/JP3920209B2/en
Priority to US12/836,161 priority patent/US8444806B2/en
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【0001】
【発明の属する技術分野】
本発明は、プラズマを用いて被処理基板の表面に堆積処理又はエッチング処理を行い半導体などの基板を製造するためのプラズマ生成装置に関する。特に、大面積に亘って均一にプラズマを発生させることにより、大面積の基板を製造する技術に関する。
【0002】
【従来の技術】
近年、アモルファスシリコン膜を用いたTFT(薄膜トランジスタ)-LCDよりも高輝度の画像を表示することができるポリシリコンTFT-LCDが注目されている。ポリシリコンTFT-LCDでは、まず、ガラス基板上にポリシリコン薄膜を形成し、マザー基板とする。このマザー基板上を多数の2次元配列された画素領域に区分し、各画素領域に薄膜トランジスタ(TFT)を形成してLCD用基板とする。大画面のポリシリコンTFT-LCDを製造するためには、高い品質、特に高い平坦性を有するポリシリコンマザー基板が必要となる。
【0003】
ポリシリコン基板は高効率の太陽電池用基板としても注目されており、需要及び応用の拡大に伴ってその大面積化が求められている。また、一般の半導体デバイス用基板についても、単結晶サイズを超える大面積のものについては、堆積によるマザー基板を使用せざるを得ない。
【0004】
これらの分野で用いられるマザー基板を製造するために、プラズマを用いた処理が行われる。プラズマを用いた処理には、土台となる被処理基板の表面にマザー基板の原料を堆積させる処理、及び、マザー基板を含む被処理基板表面をエッチングする処理等が含まれる。基板の大型化に伴い、プラズマ処理を行う装置も大型化する必要があるが、その際の最も大きな問題は、プラズマ処理の不均一性である。これを解消するためには、基板全面に亘ってプラズマ密度をできるだけ均一にする必要がある。一方、生産性の観点からは、プラズマ密度を高め、それにより堆積速度やエッチングレートを高めることが求められる。
【0005】
プラズマを生成する方法には、ECR(電子サイクロトン共鳴)プラズマ方式、マイクロ波プラズマ方式、誘導結合型プラズマ方式、容量結合型プラズマ方式等がある。このうち誘導結合型プラズマ方式は、アンテナとなる誘導コイルに高周波電圧を印加し、プラズマ生成装置の内部に誘導電磁界を生成して、それによりプラズマを生成するものである。この構成によれば、前記のプラズマ装置に求められる要件の1つである高密度のプラズマを生成することができる。一方、プラズマ密度はアンテナからの距離に依存するため、前記のもう1つの要件であるプラズマ密度の均一性についてはアンテナの形状や位置等の構成を工夫することにより向上することが図られている。例えば、特許文献1には、プラズマ生成室の天井の外側に設けた平板状のコイルから高周波を導入し、プラズマ密度の均一性を向上させることが記載されている。
【0006】
【特許文献1】
特開2000-58297号公報([0026]〜[0027]、図1)
【0007】
このような構成において基板の大面積化を図ろうとすると、プラズマ生成室天井の機械的強度を確保するために天井の壁を十分に厚くしなければならない。しかし、特許文献1の装置ではプラズマ生成室の外側にアンテナが配置されているため、アンテナから放射される誘導電磁界が壁において減衰し、プラズマ生成室内の誘導電磁界の強度を十分に得ることが困難である。即ち、特許文献1に記載の方法では、プラズマ密度の均一性については一定の向上が見られるものの、プラズマ密度を十分に高くすることは困難である。
【0008】
それに対して本願発明者らは特許文献2において、高周波アンテナをプラズマ生成室内部に設けること([0008]〜[0010])、更に複数のアンテナを設けること([0050])を提案している。
【0009】
【特許文献2】
特開2001-35697号公報([0008]〜[0010]、[0050]、図11)
【0010】
この構成によれば、プラズマ生成室の壁が障害とならないため、誘導電磁界が減衰することなくプラズマ生成室内に放射され、プラズマ密度を十分に高くすることができる。また、均等に配置された複数のアンテナから誘導電磁界が放射されるため、その均一性が向上し、それによりプラズマ密度の均一性を向上させることができる。これらの効果により、大面積の被処理基板に対する堆積処理やエッチング処理が可能になる。以下、特許文献2に記載の複数のアンテナを設ける構成を「マルチアンテナ方式」と呼ぶ。
【0011】
【発明が解決しようとする課題】
今後更に大面積の基板を処理するためには、プラズマ密度の強度を十分に確保しつつ、より均一性の高いプラズマ状態を生成することが求められる。そのためには、前記マルチアンテナ方式においても、各アンテナの形状・位置等やアンテナ間の関係等の現在考慮されていないパラメータを検討することが必要である。
【0012】
本発明はこのような課題を解決するために成されたものであり、その目的とするところは、空間的に均一で且つ高い密度のプラズマを生成することができるプラズマ生成装置を提供することにある。
【0013】
【課題を解決するための手段】
上記課題を解決するために成された本発明に係るプラズマ生成装置は、
a)真空容器と、
b)前記真空容器内に設けた、被処理基板を載置する基板台と、
c)3個以上のU 字形の高周波アンテナをその両端の電極の一方を高周波電源に接続すると共に他方を接地し且つ各高周波アンテナを前記基板台に平行であって前記真空容器内を囲うように前記真空容器の内壁面に並べて設けたマルチアンテナであって、その内の1組又は複数組の隣接アンテナの隣接電極同士を同一極性としたマルチアンテナと、
を備えることを特徴とする。
【0014】
【発明の実施の形態】
本発明に係るプラズマ生成装置は、その内部がプラズマ生成室となる真空容器を有する。真空容器は真空ポンプに接続され、真空容器内部が所定の真空度に維持される。この真空容器内部に、被処理基板を載置する基板台を設ける。また、生成するプラズマの原料となるガスを真空容器内に導入するガス導入口を設ける。
【0015】
真空容器内に、高周波アンテナを複数個設ける。高周波アンテナを配置する際には、両端の電極が基板台に平行に並ぶようにする。各高周波アンテナの一方の電極を高周波電源に接続し、他方の電極を接地する。それらの電極間に高周波電圧を印加することにより誘導電磁界を生成する。
【0016】
ここまでの構成は、特許文献2に記載の構成と同様である。本発明においては、隣接アンテナの隣接電極同士が同一極性となるようにする。即ち、隣接電極を共に高周波電源に接続するか、又は共に接地する。
【0017】
本発明において上記の構成を用いる理由を説明するために、まず特許文献2に記載の装置の隣接アンテナの隣接電極の極性について説明する。特許文献2の図11では、隣接電極同士が異なる極性となるように高周波電源及び接地に接続される。このような構成により、隣接アンテナの隣接電極間に高周波電圧が印加され、その部分のみ局所的にプラズマ密度が高くなる。そのため、例えば基板台中央部等の、その隣接電極間以外の箇所のプラズマ密度が低くなり、プラズマ密度の均一性がよくない。プラズマ密度を高めるために高周波アンテナの設置密度を高くして隣接アンテナ間の距離を狭くすると、隣接アンテナの隣接電極間に生じる電場がより強くなり、プラズマ密度の均一性が更に悪化する。
【0018】
それに対して本発明においては、隣接アンテナの隣接電極同士を同一極性とするため、その隣接電極間は常に等電位であり高周波電圧が印加されない。そのため、その隣接電極間に局所的な高プラズマ密度領域が形成されることがない。極性を同一にする電極を適宜選択することにより、プラズマ密度の分布を制御することができる。
【0019】
更に、全ての高周波アンテナの全ての隣接電極同士を同一極性とすることにより、全ての隣接電極間において、極性の違いによる電圧が生じず、高プラズマ密度領域の形成が防止される。これにより、基板部分のプラズマ密度の低下を防ぎ、真空容器内の全体に亘ってプラズマ密度の均一性を向上することができる。また、プラズマ密度の均一性を悪化させることなく隣接アンテナ間の距離を狭くし高周波アンテナの設置密度を高くすることができるため、全体としてプラズマ密度を高くすることができる。
【0020】
【発明の効果】
本発明により、大面積基板の製造が可能なマルチアンテナ方式の誘導結合型プラズマ生成装置において、基板部分のプラズマ密度をより高め、且つプラズマ密度分布をより均一化することができるようになる。また、高周波アンテナの設置密度を従来よりも高くすることが可能になり、より高密度のプラズマを生成することが可能になる。このプラズマ生成装置を用いれば、大面積の被処理基板に、均一性が高く且つ速い速度で堆積処理又はエッチング処理を行うことができ、全面に亘って高い均一性を有する基板を製造することができる。また、使用方法によっては、プラズマ密度の分布を制御することもできる。
【0021】
【実施例】
図1及び図2に、本発明に係るプラズマ生成装置の一実施例の構成を示す。図1は鉛直方向の断面図であり、図2は平面図である。真空容器11の内部が本プラズマ生成装置のプラズマ生成室となる。真空容器11内部の水平方向の断面は、長辺130cm、短辺100cmの矩形である。真空容器11には真空ポンプ(図示せず)を接続する。真空容器11内に被処理基板13を載置するための、長辺94cm、短辺76cmの矩形の平面状の基板台14を設ける。基板台14は、その下部に設けた昇降部141により昇降可能となっている。また、真空容器11の下側部には被処理基板13を出し入れするための基板出入口12を設ける。真空容器11内上部には、内壁に沿って水平に真空容器11内を一周分周回する周回部と、真空容器11外部に接続する接続部から成るガスパイプ15を設ける。このガスパイプ15の周回部の表面には、多数の孔を、真空容器11内に均等にガスを導入するために適宜分布で配置する。
【0022】
真空容器11の4つの側壁のうちその水平方向に長い方の2面には4個ずつ、短い方の2面には3個ずつ等間隔に高周波アンテナ16を設ける。高周波アンテナ16の基板台14からの高さは18cmである。以下においては、同一の側壁に設ける3個又は4個の高周波アンテナを1組のアンテナ群として説明する。図2には、アンテナ群の例として3個の高周波アンテナから成るアンテナ群191及び4個の高周波アンテナから成るアンテナ群192を示す。個々の高周波アンテナ16の形状はU字形である。本実施例の高周波アンテナは、側壁に平行な方向の辺の長さを15cmとする。同一のアンテナ群内において隣接する高周波アンテナ同士の隙間を、水平方向に長い方の側壁においては8.0cm、短い方の側壁においては9.5cmとする。これらの高周波アンテナの個数、大きさ及び間隔は、製造する基板の形状や面積及び真空容器11内部の水平方向の断面の形状や断面積に応じて適宜設定する。
【0023】
各アンテナ群に1台ずつ高周波電源18を設ける。各高周波アンテナ16の2つの電極のうち、一方はインピーダンス整合器17を介して高周波電源18に接続し、他方は接地する。同一のアンテナ群内では、隣接する高周波アンテナ同士において隣接電極同士を同極性とする。例えばアンテナ群191では、隣接する高周波アンテナ161と高周波アンテナ162においては互いに隣接する側の電極を共にインピーダンス整合器17−高周波電源18に接続し、高周波アンテナ162と高周波アンテナ163においては互いに隣接する側の電極を共に接地する。
【0024】
本実施例のプラズマ生成装置の動作を説明する。昇降部141を動作させて基板台14を降下させる。被処理基板13を基板出入口12から真空容器11内に入れ、基板台14上に載置した後、基板台14を所定の位置まで上昇させる。プラズマの原料ガスを所定のガス圧でガスパイプ15に導入し、4台の高周波電源18から所定の高周波電力を各高周波アンテナ16に供給する。これにより、各高周波アンテナ16が誘導電界を生成する。
【0025】
隣接アンテナ同士の隣接電極を同極性とすることにより、図3(a)に示す隣接アンテナ間の隙間20においてこれらの電極間に電位差が生じることはない。このため、この隙間20において端子間電位差の存在によりプラズマ濃度が上昇することを防ぎ、その他の部分のプラズマ濃度が低下することを防ぐことができる。これによって、プラズマ濃度の空間分布の均一性を更に高めることができる。
【0026】
この均一性の高い誘導電界によって、真空容器11内に導入されたガスが電離して空間分布の均一性の高いプラズマが生成される。このプラズマによって、大面積の被処理基板13の全面に亘り均一性の高い堆積処理又はエッチング処理を行うことができる。
【0027】
本実施例に対する比較例であるプラズマ生成装置の平面図を図4に示す。この比較例においては、隣接する高周波アンテナ同士において互いに近接する側の端子を逆極性とする。例えば隣接する高周波アンテナ161と高周波アンテナ162においては、高周波アンテナ161では高周波アンテナ162に近接する側の端子を接地側に、高周波アンテナ162では高周波アンテナ161に近接する側の端子をインピーダンス整合器17−高周波電源18に接続する。端子の極性以外は、図2の本実施例と同一の構成とする。
【0028】
この比較例においては、図3(b)に示すように、隙間20において電極間に電位差が生じる。このため、この隙間20におけるプラズマ濃度が他の位置よりも高くなる。また、それに伴って他の位置のプラズマ濃度が低下する。
【0029】
以下に、上記本実施例のプラズマ生成装置において生成されるプラズマの密度を測定した結果を示す。併せて、上記比較例のプラズマ生成装置おいて生成されるプラズマの密度を示し、本実施例との比較を行う。本測定におけるプラズマ生成条件は以下の通りである。生成するプラズマはArプラズマである。あらかじめ真空容器11内を5×10-5Paまで排気した後、原料ガスであるArガスを1.33Paのガス圧まで供給する。各高周波アンテナ16に周波数13.56MHzの高周波電力を供給する。その他の条件は各測定の説明の際に示す。また、プラズマ密度の測定にはラングミュアプローブ法を用いた。
【0030】
図5に、高周波アンテナと同じ高さであって基板台中央の直上におけるプラズマ密度を測定した結果を示す。ここで、縦軸は対数スケールで表したプラズマ電子密度であり、横軸は各高周波電源が供給する高周波電力の大きさである。高周波電力の値がいずれの場合も、本実施例の装置の方が比較例の装置よりも高いプラズマ密度を得ることができる。特に、高周波電力が1200W〜2500Wの場合、本実施例のプラズマ密度は比較例のプラズマ密度の約2倍となる。
【0031】
図6に、プラズマ密度の空間分布を測定した結果を示す。その際の測定条件は以下の通りである。高周波電力は、図2及び図4に示す1組のアンテナ群192にのみ供給する。高周波電源が供給する高周波電力の大きさは1500Wである。プラズマ密度の測定点である図6の横軸は、アンテナ群192を設けた側壁に平行に13cm離れた直線上の位置を表す。
【0032】
図6より、比較例のプラズマ生成装置においては、端部のプラズマ密度が中心付近のプラズマ密度よりも低くなり、プラズマ密度の空間分布の偏りが見られる。それに対して本実施例のプラズマ生成装置においては、プラズマ密度の空間分布の偏りが比較例のプラズマ生成装置におけるそれよりも小さくなり、プラズマ密度分布の均一性が改善される。
【図面の簡単な説明】
【図1】 本発明に係るプラズマ生成装置の一実施例の鉛直方向の断面図。
【図2】 図1のプラズマ生成装置の平面図。
【図3】 隣接アンテナ間の隙間及びその間における電位差についての説明図。
【図4】 比較例のプラズマ生成装置の平面図。
【図5】 図2の本発明のプラズマ生成装置及び図4の比較例のプラズマ生成装置における、装置中央のプラズマ密度を示すグラフ。
【図6】 図2の本発明のプラズマ生成装置及び図4の比較例のプラズマ生成装置における、プラズマ密度の空間分布を示すグラフ。
【符号の説明】
11…真空容器
12…基板搬出入口
13…被処理基板
14…基板台
141…昇降部
15…ガスパイプ
16、161、162、163…高周波アンテナ
17…インピーダンス整合器
18…高周波電源
191、192…アンテナ群
20…隙間
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a plasma generation apparatus for manufacturing a substrate such as a semiconductor by performing a deposition process or an etching process on a surface of a substrate to be processed using plasma. In particular, the present invention relates to a technique for manufacturing a large area substrate by generating plasma uniformly over a large area.
[0002]
[Prior art]
In recent years, attention has been paid to a polysilicon TFT-LCD capable of displaying an image with higher brightness than a TFT (thin film transistor) -LCD using an amorphous silicon film. In a polysilicon TFT-LCD, first, a polysilicon thin film is formed on a glass substrate to form a mother substrate. The mother substrate is divided into a number of two-dimensionally arranged pixel regions, and a thin film transistor (TFT) is formed in each pixel region to form an LCD substrate. In order to manufacture a large-screen polysilicon TFT-LCD, a polysilicon mother substrate having high quality, particularly high flatness is required.
[0003]
The polysilicon substrate is also attracting attention as a highly efficient solar cell substrate, and is required to have a large area as demand and application expand. In addition, as for a general semiconductor device substrate, a mother substrate obtained by deposition must be used for a large area exceeding the single crystal size.
[0004]
In order to manufacture a mother substrate used in these fields, a process using plasma is performed. The process using plasma includes a process of depositing a raw material of the mother substrate on the surface of the substrate to be processed which is a base, a process of etching the surface of the substrate to be processed including the mother substrate, and the like. Along with the increase in size of the substrate, it is necessary to increase the size of the apparatus for performing the plasma treatment. The biggest problem at that time is the nonuniformity of the plasma treatment. In order to solve this, it is necessary to make the plasma density as uniform as possible over the entire surface of the substrate. On the other hand, from the viewpoint of productivity, it is required to increase the plasma density, thereby increasing the deposition rate and the etching rate.
[0005]
As a method for generating plasma, there are an ECR (electron cycloton resonance) plasma method, a microwave plasma method, an inductively coupled plasma method, a capacitively coupled plasma method, and the like. Among them, the inductively coupled plasma method is a method in which a high frequency voltage is applied to an induction coil serving as an antenna, an induction electromagnetic field is generated inside the plasma generator, and plasma is thereby generated. According to this configuration, it is possible to generate high-density plasma, which is one of the requirements for the plasma apparatus. On the other hand, since the plasma density depends on the distance from the antenna, the plasma density uniformity, which is another requirement, is improved by devising the configuration of the antenna shape and position. . For example, Patent Document 1 describes that high frequency is introduced from a flat coil provided outside the ceiling of a plasma generation chamber to improve the uniformity of plasma density.
[0006]
[Patent Document 1]
JP 2000-58297 A ([0026] to [0027], FIG. 1)
[0007]
In order to increase the area of the substrate in such a configuration, the ceiling wall must be made sufficiently thick in order to ensure the mechanical strength of the plasma generation chamber ceiling. However, since the antenna is arranged outside the plasma generation chamber in the apparatus of Patent Document 1, the induction electromagnetic field radiated from the antenna is attenuated on the wall, and the strength of the induction electromagnetic field in the plasma generation chamber can be sufficiently obtained. Is difficult. That is, with the method described in Patent Document 1, it is difficult to make the plasma density sufficiently high, although a certain improvement is seen in the uniformity of the plasma density.
[0008]
On the other hand, the inventors of the present application have proposed to provide a high-frequency antenna in the plasma generation chamber ([0008] to [0010]) and further provide a plurality of antennas ([0050]). .
[0009]
[Patent Document 2]
Japanese Patent Laid-Open No. 2001-35697 ([0008] to [0010], [0050], FIG. 11)
[0010]
According to this configuration, since the wall of the plasma generation chamber does not become an obstacle, the induction electromagnetic field is radiated into the plasma generation chamber without attenuation, and the plasma density can be sufficiently increased. In addition, since the induction electromagnetic field is radiated from a plurality of antennas arranged evenly, the uniformity thereof can be improved, thereby improving the uniformity of the plasma density. Due to these effects, it is possible to perform a deposition process or an etching process on a substrate to be processed having a large area. Hereinafter, a configuration provided with a plurality of antennas described in Patent Document 2 is referred to as a “multi-antenna method”.
[0011]
[Problems to be solved by the invention]
In order to process a substrate having a larger area in the future, it is required to generate a plasma state with higher uniformity while ensuring a sufficient plasma density intensity. To that end, even in the multi-antenna method, it is necessary to examine parameters that are not currently considered, such as the shape and position of each antenna and the relationship between antennas.
[0012]
The present invention has been made to solve such problems, and an object of the present invention is to provide a plasma generation apparatus capable of generating a spatially uniform and high density plasma. is there.
[0013]
[Means for Solving the Problems]
A plasma generation apparatus according to the present invention, which has been made to solve the above problems,
a) a vacuum vessel;
b) a substrate base on which a substrate to be processed is placed, provided in the vacuum vessel;
c) three or more U-shaped high frequency antenna, a grounded and each radio-frequency antenna and the other parallel to the substrate table so as to surround said vacuum container with connecting one of the ends of the electrodes to a high frequency power supply a multi-antenna a multi-antenna, in which the adjacent electrodes of one or more sets of adjacent antennas of the same polarity arranged side by side on the inner wall surface of the vacuum container,
It is characterized by providing.
[0014]
DETAILED DESCRIPTION OF THE INVENTION
The plasma generation apparatus according to the present invention has a vacuum container whose inside is a plasma generation chamber. The vacuum vessel is connected to a vacuum pump, and the inside of the vacuum vessel is maintained at a predetermined degree of vacuum. A substrate stand on which the substrate to be processed is placed is provided inside the vacuum container. In addition, a gas introduction port is provided for introducing a gas as a raw material of the plasma to be generated into the vacuum vessel.
[0015]
A plurality of high-frequency antennas are provided in the vacuum vessel. When arranging the high-frequency antenna, the electrodes at both ends are arranged in parallel to the substrate table. One electrode of each high-frequency antenna is connected to a high-frequency power source, and the other electrode is grounded. An induction electromagnetic field is generated by applying a high-frequency voltage between these electrodes.
[0016]
The configuration so far is the same as the configuration described in Patent Document 2. In the present invention, adjacent electrodes of adjacent antennas have the same polarity. That is, both adjacent electrodes are connected to a high frequency power source or both are grounded.
[0017]
In order to explain the reason why the above configuration is used in the present invention, first, the polarity of the adjacent electrode of the adjacent antenna of the apparatus described in Patent Document 2 will be described. In FIG. 11 of Patent Document 2, the adjacent electrodes are connected to a high-frequency power source and ground so as to have different polarities. With such a configuration, a high frequency voltage is applied between the adjacent electrodes of the adjacent antenna, and the plasma density is locally increased only in that portion. For this reason, for example, the plasma density at a portion other than between the adjacent electrodes such as the central portion of the substrate base is lowered, and the uniformity of the plasma density is not good. If the installation density of the high-frequency antenna is increased to increase the plasma density and the distance between the adjacent antennas is reduced, the electric field generated between the adjacent electrodes of the adjacent antenna becomes stronger, and the uniformity of the plasma density is further deteriorated.
[0018]
On the other hand, in the present invention, since adjacent electrodes of adjacent antennas have the same polarity, the adjacent electrodes are always equipotential and no high frequency voltage is applied. Therefore, a local high plasma density region is not formed between the adjacent electrodes. The plasma density distribution can be controlled by appropriately selecting electrodes having the same polarity.
[0019]
Furthermore, by setting all the adjacent electrodes of all the high-frequency antennas to the same polarity, a voltage due to the difference in polarity does not occur between all the adjacent electrodes, and formation of a high plasma density region is prevented. Thereby, the fall of the plasma density of a board | substrate part can be prevented, and the uniformity of a plasma density can be improved over the inside in a vacuum vessel. In addition, since the distance between adjacent antennas can be reduced and the installation density of the high-frequency antenna can be increased without deteriorating the uniformity of the plasma density, the plasma density can be increased as a whole.
[0020]
【The invention's effect】
According to the present invention, in a multi-antenna type inductively coupled plasma generating apparatus capable of manufacturing a large area substrate, the plasma density of the substrate portion can be further increased and the plasma density distribution can be made more uniform. Further, the installation density of the high-frequency antenna can be increased as compared with the prior art, and higher density plasma can be generated. By using this plasma generation apparatus, it is possible to perform deposition processing or etching processing on a large area substrate to be processed with high uniformity and at a high speed, and to manufacture a substrate having high uniformity over the entire surface. it can. Further, depending on the method of use, the plasma density distribution can be controlled.
[0021]
【Example】
1 and 2 show the configuration of an embodiment of the plasma generating apparatus according to the present invention. 1 is a vertical sectional view, and FIG. 2 is a plan view. The inside of the vacuum vessel 11 becomes a plasma generation chamber of the present plasma generation apparatus. The horizontal cross section inside the vacuum vessel 11 is a rectangle having a long side of 130 cm and a short side of 100 cm. A vacuum pump (not shown) is connected to the vacuum vessel 11. A rectangular planar substrate table 14 having a long side of 94 cm and a short side of 76 cm for mounting the substrate to be processed 13 in the vacuum vessel 11 is provided. The substrate table 14 can be moved up and down by a lifting unit 141 provided in the lower part thereof. In addition, a substrate inlet / outlet 12 is provided on the lower side of the vacuum vessel 11 for taking in and out the substrate 13 to be processed. In the upper part of the vacuum vessel 11, there is provided a gas pipe 15 including a circulating portion that circulates around the vacuum vessel 11 horizontally along the inner wall and a connection portion connected to the outside of the vacuum vessel 11. A large number of holes are arranged on the surface of the circulating portion of the gas pipe 15 in an appropriate distribution in order to introduce gas evenly into the vacuum vessel 11.
[0022]
Among the four side walls of the vacuum vessel 11, four high frequency antennas 16 are provided at equal intervals on each of the two longer surfaces in the horizontal direction and three on the shorter two surfaces. The height of the high frequency antenna 16 from the substrate table 14 is 18 cm. Hereinafter, three or four high-frequency antennas provided on the same side wall will be described as a set of antenna groups. FIG. 2 shows an antenna group 191 composed of three high-frequency antennas and an antenna group 192 composed of four high-frequency antennas as examples of the antenna group. The shape of each high frequency antenna 16 is U-shaped. In the high-frequency antenna of this embodiment, the length of the side in the direction parallel to the side wall is 15 cm. The gap between adjacent high frequency antennas in the same antenna group is set to 8.0 cm on the longer side wall in the horizontal direction and 9.5 cm on the shorter side wall. The number, size, and interval of these high-frequency antennas are appropriately set according to the shape and area of the substrate to be manufactured and the shape and cross-sectional area of the horizontal section inside the vacuum vessel 11.
[0023]
One high frequency power supply 18 is provided for each antenna group. One of the two electrodes of each high-frequency antenna 16 is connected to the high-frequency power source 18 via the impedance matching unit 17 and the other is grounded. In the same antenna group, adjacent electrodes have the same polarity in adjacent high frequency antennas. For example, in the antenna group 191, in the adjacent high-frequency antenna 161 and the high-frequency antenna 162, the electrodes adjacent to each other are both connected to the impedance matching unit 17-the high-frequency power source 18, and the high-frequency antenna 162 and the high-frequency antenna 163 are adjacent to each other. Are grounded together.
[0024]
The operation of the plasma generating apparatus of this embodiment will be described. The raising / lowering unit 141 is operated to lower the substrate table 14. The substrate 13 to be processed is put into the vacuum container 11 from the substrate entrance 12 and placed on the substrate table 14, and then the substrate table 14 is raised to a predetermined position. A plasma source gas is introduced into the gas pipe 15 at a predetermined gas pressure, and predetermined high-frequency power is supplied to each high-frequency antenna 16 from four high-frequency power sources 18. Thereby, each high frequency antenna 16 produces | generates an induction electric field.
[0025]
By setting the adjacent electrodes of the adjacent antennas to have the same polarity, no potential difference is generated between these electrodes in the gap 20 between the adjacent antennas shown in FIG. For this reason, it is possible to prevent the plasma concentration from increasing due to the presence of the potential difference between the terminals in the gap 20 and to prevent the plasma concentration from decreasing in other portions. Thereby, the uniformity of the spatial distribution of the plasma concentration can be further improved.
[0026]
Due to this highly uniform induced electric field, the gas introduced into the vacuum vessel 11 is ionized to generate plasma with high spatial distribution. By this plasma, a highly uniform deposition process or etching process can be performed over the entire surface of the substrate 13 having a large area.
[0027]
FIG. 4 shows a plan view of a plasma generating apparatus which is a comparative example with respect to the present embodiment. In this comparative example, terminals adjacent to each other in adjacent high-frequency antennas have opposite polarities. For example, in the adjacent high-frequency antenna 161 and high-frequency antenna 162, the terminal close to the high-frequency antenna 162 is connected to the ground side in the high-frequency antenna 161, and the terminal close to the high-frequency antenna 161 is connected to the impedance matcher 17- Connected to a high frequency power supply 18. Except for the polarity of the terminals, the configuration is the same as that of the present embodiment of FIG.
[0028]
In this comparative example, as shown in FIG. 3B, a potential difference is generated between the electrodes in the gap 20. For this reason, the plasma concentration in the gap 20 becomes higher than other positions. In addition, the plasma concentration at other positions decreases accordingly.
[0029]
Below, the result of having measured the density of the plasma produced | generated in the plasma production apparatus of the said Example is shown. In addition, the density of plasma generated in the plasma generation apparatus of the comparative example is shown and compared with the present embodiment. The plasma generation conditions in this measurement are as follows. The generated plasma is Ar plasma. The inside of the vacuum vessel 11 is evacuated to 5 × 10 −5 Pa in advance, and then Ar gas as a raw material gas is supplied to a gas pressure of 1.33 Pa. High frequency power having a frequency of 13.56 MHz is supplied to each high frequency antenna 16. Other conditions are shown in the description of each measurement. The Langmuir probe method was used to measure the plasma density.
[0030]
FIG. 5 shows the result of measuring the plasma density at the same height as the high-frequency antenna and directly above the center of the substrate table. Here, the vertical axis represents the plasma electron density expressed in a logarithmic scale, and the horizontal axis represents the magnitude of the high-frequency power supplied from each high-frequency power source. Regardless of the value of the high-frequency power, the apparatus of this embodiment can obtain a higher plasma density than the apparatus of the comparative example. In particular, when the high-frequency power is 1200 W to 2500 W, the plasma density of this example is about twice that of the comparative example.
[0031]
FIG. 6 shows the result of measuring the spatial distribution of plasma density. The measurement conditions at that time are as follows. The high frequency power is supplied only to a set of antenna groups 192 shown in FIGS. The magnitude of the high frequency power supplied from the high frequency power supply is 1500W. The horizontal axis of FIG. 6 which is a measurement point of the plasma density represents a position on a straight line 13 cm away from the side wall provided with the antenna group 192 in parallel.
[0032]
As shown in FIG. 6, in the plasma generating apparatus of the comparative example, the plasma density at the end is lower than the plasma density near the center, and the spatial distribution of the plasma density is biased. On the other hand, in the plasma generation apparatus of the present embodiment, the deviation of the spatial distribution of the plasma density is smaller than that in the plasma generation apparatus of the comparative example, and the uniformity of the plasma density distribution is improved.
[Brief description of the drawings]
FIG. 1 is a vertical sectional view of an embodiment of a plasma generating apparatus according to the present invention.
FIG. 2 is a plan view of the plasma generation apparatus of FIG.
FIG. 3 is an explanatory diagram of a gap between adjacent antennas and a potential difference therebetween.
FIG. 4 is a plan view of a plasma generation apparatus of a comparative example.
5 is a graph showing the plasma density at the center of the apparatus in the plasma generation apparatus of the present invention in FIG. 2 and the plasma generation apparatus in the comparative example in FIG. 4;
6 is a graph showing a plasma density spatial distribution in the plasma generation apparatus of the present invention of FIG. 2 and the plasma generation apparatus of the comparative example of FIG. 4;
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 11 ... Vacuum container 12 ... Substrate carrying in / out port 13 ... Processed substrate 14 ... Substrate stand 141 ... Elevating part 15 ... Gas pipe 16, 161, 162, 163 ... High frequency antenna 17 ... Impedance matching device 18 ... High frequency power supply 191, 192 ... Antenna group 20 ... Gap

Claims (5)

a)真空容器と、
b)前記真空容器内に設けた、被処理基板を載置する基板台と、
c)3個以上のU 字形の高周波アンテナをその両端の電極の一方を高周波電源に接続すると共に他方を接地し且つ各高周波アンテナを前記基板台に平行であって前記真空容器内を囲うように前記真空容器の内壁面に並べて設けたマルチアンテナであって、前記高周波アンテナの内の1組又は複数組の隣接アンテナの隣接電極同士を同一極性としたマルチアンテナと、
を備えることを特徴とするプラズマ生成装置。
a) a vacuum vessel;
b) a substrate base on which a substrate to be processed is placed, provided in the vacuum vessel;
c) three or more U-shaped high frequency antenna, a grounded and each radio-frequency antenna and the other parallel to the substrate table so as to surround said vacuum container with connecting one of the ends of the electrodes to a high frequency power supply a multi-antenna wherein a multi-antenna provided side by side on the inner wall surface of the vacuum chamber, where the adjacent electrodes of one or more sets of adjacent antennas of said high frequency antenna to the same polarity,
A plasma generating apparatus comprising:
全ての高周波アンテナにおいて、隣接アンテナの隣接電極同士を同一極性としたことを特徴とする請求項1に記載のプラズマ生成装置。  The plasma generating apparatus according to claim 1, wherein adjacent electrodes of adjacent antennas have the same polarity in all high-frequency antennas. 真空容器内に、3個以上のU 字形高周波アンテナをその両端の電極の一方を高周波電源に接続すると共に他方を接地し且つ各高周波アンテナを前記基板台に平行であって前記真空容器内を囲うように前記真空容器の内壁面に並べて設けたマルチアンテナを備えるプラズマ生成装置を用いた基板製造方法において、前記高周波アンテナの内の1組又は複数組の隣接アンテナの隣接電極同士を同一極性とすることにより、前記プラズマ生成装置内のプラズマ密度分布を制御することを特徴とする基板製造方法。In the vacuum vessel, three or more U- shaped high-frequency antennas , one of the electrodes at both ends thereof is connected to a high-frequency power source, the other is grounded, and each high-frequency antenna is parallel to the substrate table and is placed in the vacuum vessel. In a substrate manufacturing method using a plasma generating apparatus provided with a multi-antenna arranged side by side on an inner wall surface of the vacuum vessel so as to surround, the adjacent electrodes of one set or a plurality of sets of adjacent antennas of the high-frequency antenna have the same polarity By doing so, the plasma density distribution in the said plasma production | generation apparatus is controlled, The board | substrate manufacturing method characterized by the above-mentioned. 全ての高周波アンテナにおいて、隣接アンテナの隣接電極同士を同一極性とすることを特徴とする請求項3に記載の基板製造方法。  4. The substrate manufacturing method according to claim 3, wherein adjacent electrodes of adjacent antennas have the same polarity in all high-frequency antennas. 真空容器内に、3個以上のU 字形高周波アンテナをその両端の電極の一方を高周波電源に接続すると共に他方を接地し且つ各高周波アンテナを前記基板台に平行であって前記真空容器内を囲うように前記真空容器の内壁面に並べて設けたマルチアンテナを備えるプラズマ生成装置において、前記高周波アンテナの内の1組又は複数組の隣接アンテナの隣接電極同士を同一極性とすることにより、前記プラズマ生成装置内のプラズマ密度分布を制御することを特徴とするプラズマ制御方法。In the vacuum vessel, three or more U- shaped high-frequency antennas , one of the electrodes at both ends thereof is connected to a high-frequency power source, the other is grounded, and each high-frequency antenna is parallel to the substrate table and is placed in the vacuum vessel. In the plasma generating apparatus including a multi-antenna arranged side by side on the inner wall surface of the vacuum vessel so as to surround , the plasma is obtained by setting adjacent electrodes of one or more sets of adjacent antennas of the high-frequency antenna to the same polarity. A plasma control method for controlling a plasma density distribution in a generation apparatus.
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TW099122626A TW201041455A (en) 2002-12-16 2003-12-11 Plasma generation device, plasma control method, and substrate manufacturing method
TW092135000A TW200420201A (en) 2002-12-16 2003-12-11 Plasma generation device, plasma control method and substrate manufacturing method
KR1020057011022A KR101090726B1 (en) 2002-12-16 2003-12-12 Plasma generation device plasma control method and substrate manufacturing method
US10/539,254 US7785441B2 (en) 2002-12-16 2003-12-12 Plasma generator, plasma control method, and method of producing substrate
CN2007101624036A CN101128084B (en) 2002-12-16 2003-12-12 Plasma generation device, plasma control method, and substrate manufacturing method
EP03780748.4A EP1575343B1 (en) 2002-12-16 2003-12-12 Plasma generation device, plasma control method, and substrate manufacturing method
CN2007101624017A CN101128083B (en) 2002-12-16 2003-12-12 Plasma generation device, plasma control method, and substrate manufacturing method
PCT/JP2003/016007 WO2004056159A1 (en) 2002-12-16 2003-12-12 Plasma generation device, plasma control method, and substrate manufacturing method
EP10180427.6A EP2259663B1 (en) 2002-12-16 2003-12-12 Plasma generator, plasma control method and method of producing substrate
KR1020117019924A KR101186822B1 (en) 2002-12-16 2003-12-12 Plasma generation device, plasma control method, and substrate manufacturing method
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