JP2001140085A - Plasma treating system - Google Patents
Plasma treating systemInfo
- Publication number
- JP2001140085A JP2001140085A JP2000145470A JP2000145470A JP2001140085A JP 2001140085 A JP2001140085 A JP 2001140085A JP 2000145470 A JP2000145470 A JP 2000145470A JP 2000145470 A JP2000145470 A JP 2000145470A JP 2001140085 A JP2001140085 A JP 2001140085A
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- Prior art keywords
- frequency
- vacuum chamber
- electrode
- common
- vacuum
- 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.)
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Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、一つの真空チャン
バー内に複数の電極を設け、各電極にそれぞれ処理すべ
き基板を装着し、真空チャンバー内に発生されたプラズ
マを利用して例えばエッチング、スパッタリングまたは
化学気相成長(化学蒸着)などの所定の処理を行うよう
にしたプラズマ処理装置に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention provides a plurality of electrodes in one vacuum chamber, mounts a substrate to be processed on each electrode, and performs etching, for example, by using plasma generated in the vacuum chamber. The present invention relates to a plasma processing apparatus that performs a predetermined process such as sputtering or chemical vapor deposition (chemical vapor deposition).
【0002】[0002]
【従来の技術】近年、半導体や電子部品における薄膜形
成や機能膜形成、パターン形成にプラズマを利用した種
々の装置が用いられている。添付図面の図4にはこの種
の装置の従来例を示し、Aは真空チャンバーで、その中
に複数の基板電極Bがそれぞれの対向電極Cと対を成し
て配列されている。各基板電極Bはマッチング回路網D
を介してそれぞれの高周波励起電源Eに接続されてい
る。なお、各対向電極Cは図示したようにそれぞれ接地
されている。2. Description of the Related Art In recent years, various apparatuses using plasma for forming thin films, functional films, and patterns in semiconductors and electronic parts have been used. FIG. 4 of the accompanying drawings shows a conventional example of this type of apparatus, in which A is a vacuum chamber in which a plurality of substrate electrodes B are arranged in pairs with respective counter electrodes C. Each substrate electrode B is a matching network D
Are connected to the respective high-frequency excitation power supplies E. Each counter electrode C is grounded as shown.
【0003】[0003]
【発明が解決しようとする課題】このような従来の装置
においては、生産性の観点では満足されるが、真空チャ
ンバー内に設けられる基板電極の数だけマッチング回路
網及び高周波励起電源を設ける必要がある。そのため高
周波電極の設けられる数が増えれば増える程、マッチン
グ回路網及び高周波励起電源の使用される数が増え、そ
の分、装置のコストが嵩むことになる。このようにこの
種の従来の装置は、設備に掛かるコストが高く、低コス
ト化が求められている。Although such a conventional apparatus is satisfactory from the viewpoint of productivity, it is necessary to provide matching circuits and high-frequency excitation power supplies by the number of substrate electrodes provided in the vacuum chamber. is there. Therefore, as the number of high-frequency electrodes provided increases, the number of matching circuits and high-frequency excitation power supplies used increases, and the cost of the apparatus increases accordingly. As described above, this type of conventional apparatus has a high facility cost and is required to be reduced in cost.
【0004】そこで、装置のコストを低減するために、
真空チャンバー内に設けられる複数の高周波電極を共通
のマッチング回路網及び高周波励起電源に接続すること
も考えられるが、そのように構成すると、それぞれの電
極容量及び電極を装着している接続板(通常銅製)のイン
ダクタンスのばらつきのために一番インピーダンスの低
下する電極に放電が集中し、パワー分配が不均一とな
り、高周波励起の利点である安定したプラズマの生成が
困難となる。[0004] In order to reduce the cost of the apparatus,
It is conceivable to connect a plurality of high-frequency electrodes provided in a vacuum chamber to a common matching network and a high-frequency excitation power supply.However, in such a configuration, a connection plate (normally, Dispersion of the inductance of copper (copper) causes discharge to concentrate on the electrode having the lowest impedance, resulting in non-uniform power distribution, making it difficult to generate stable plasma, which is an advantage of high-frequency excitation.
【0005】このような従来技術の問題点を解決するた
めに、本発明は、真空チャンバー内に設けられる高周波
電極の数に関わらず、装置の本来の機能を維持しながら
使用するマッチング回路網及び高周波励起電源の数を可
及的に低減できるプラズマ処理装置を提供することを目
的としている。In order to solve the problems of the prior art, the present invention provides a matching network and a matching network used while maintaining the original function of the apparatus, regardless of the number of high-frequency electrodes provided in the vacuum chamber. It is an object of the present invention to provide a plasma processing apparatus capable of reducing the number of high-frequency excitation power supplies as much as possible.
【0006】上記目的を達成するために、本発明によれ
ば、 一つの真空チャンバー内に設けられた複数の高周
波電極のそれぞれに処理すべき基板を装着し、真空チャ
ンバー内に発生されたプラズマを利用して所定の処理を
行うようにしたプラズマ処理装置において、真空チャン
バー内に設けられた複数の高周波電極をそれぞれ真空コ
ンデンサ及び共通のマッチング回路網を介して共通の電
源に接続したことを特徴としている。In order to achieve the above object, according to the present invention, a substrate to be processed is mounted on each of a plurality of high-frequency electrodes provided in one vacuum chamber, and plasma generated in the vacuum chamber is supplied. In a plasma processing apparatus configured to perform predetermined processing by utilizing, a plurality of high-frequency electrodes provided in a vacuum chamber are connected to a common power supply via a vacuum capacitor and a common matching network, respectively. I have.
【0007】また、本発明によれば、 一つの真空チャ
ンバー内に設けられた複数の高周波電極のそれぞれに処
理すべき基板を装着し、真空チャンバー内に発生された
プラズマを利用して所定の処理を行うようにしたプラズ
マ処理装置において、真空チャンバー内に設けられた複
数の高周波電極をそれぞれLC回路及び共通のマッチング
回路網を介して共通の電源に接続したことを特徴として
いる。Further, according to the present invention, a substrate to be processed is mounted on each of a plurality of high-frequency electrodes provided in one vacuum chamber, and a predetermined processing is performed by utilizing plasma generated in the vacuum chamber. Is characterized in that a plurality of high-frequency electrodes provided in a vacuum chamber are connected to a common power supply via an LC circuit and a common matching network.
【0008】本発明において、それぞれの高周波電極に
接続された真空コンデンサまたはLC回路は、装置の製作
上伴い得る高周波電極の容量のばらつき及び高周波電極
の装着される接続基体のインダクタンスのばらつきを補
正してそれぞれの高周波電極に高周波電力が均一に分配
されるように機能する。In the present invention, the vacuum capacitor or the LC circuit connected to each high-frequency electrode corrects variations in capacitance of the high-frequency electrode and variations in inductance of the connection base to which the high-frequency electrode is attached, which may occur in manufacturing the device. Thus, it functions so that high-frequency power is uniformly distributed to each high-frequency electrode.
【0009】真空チャンバー内に設けられる高周波電極
の数が比較的多い場合には、高周波電極は、それぞれ複
数の高周波電極を含む複数のグループに分けられ、各グ
ループにおける複数の高周波電極はそれぞれの真空コン
デンサまたはLC回路及び共通のマッチング回路網を介し
て共通の高周波電源に接続され得る。また、好ましく
は、各高周波電極に接続される真空コンデンサは可変真
空コンデンサから成り得る。When the number of high-frequency electrodes provided in the vacuum chamber is relatively large, the high-frequency electrodes are divided into a plurality of groups each including a plurality of high-frequency electrodes. It can be connected to a common high frequency power supply via a capacitor or LC circuit and a common matching network. Also, preferably, the vacuum condenser connected to each high-frequency electrode may be composed of a variable vacuum condenser.
【0010】[0010]
【発明の実施の形態】以下、添付図面の図1〜図3を参照
して本発明の実施の形態を説明する。図1には、本発明
をプラズマエッチング装置として実施している一つの形
態を概略的に示す。1は図示していない排気系及び放電
用ガスに接続された真空チャンバーであり、この真空チ
ャンバー1の下側壁には四つの基板電極すなわちカソー
ド電極を構成する高周波電極2が設けられ、これら四つ
の高周波電極2に対向して真空チャンバー1の上側壁に
沿って共通のアノード電極3が設けられ、この対向電極
3は接地されている。高周波電極2の各々は可変真空コ
ンデンサ4を介して共通のマッチング回路網5及び共通の
高周波電源6に接続されている。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to FIGS. FIG. 1 schematically shows one embodiment in which the present invention is implemented as a plasma etching apparatus. Reference numeral 1 denotes a vacuum chamber connected to an exhaust system and a discharge gas (not shown), and a lower wall of the vacuum chamber 1 is provided with four substrate electrodes, that is, a high-frequency electrode 2 constituting a cathode electrode. A common anode electrode 3 is provided along the upper side wall of the vacuum chamber 1 so as to face the high-frequency electrode 2, and the counter electrode 3 is grounded. Each of the high-frequency electrodes 2 is connected to a common matching network 5 and a common high-frequency power source 6 via a variable vacuum capacitor 4.
【0011】なお、図示実施の形態において、高周波電
極2の数は、単に例示のためのものであり、当然二つま
たは三つ或いは四つ以上でもよい。また各真空コンデン
サ4は可変型の代りに固定型のものでもよい。In the illustrated embodiment, the number of high-frequency electrodes 2 is merely for illustrative purposes, and may be two, three, four or more. Each vacuum condenser 4 may be a fixed type instead of a variable type.
【0012】図示実施の形態において、高周波電極2の
電極容量をCi(i=1〜4)とし、可変真空コンデン
サ4の容量をCi'(i=1〜4)とし、高周波電極2の
装着されている銅製の接続基体(図示してしない)のイ
ンダクタンスをLi(i=1〜4)とすると、それぞれ
の高周波電極2におけるインピーダンスZi(i=1〜
4)は Zi=jωLi+1/(Ci+Ci') で表される。ここでZ1=Z2=Z3=Z4となるよう
に、可変真空コンデンサ4の容量Ci'(i=1〜4)を
設定する。これにより高周波電極2全体にわたつて均一
に高周波電力が分配されることになる。In the illustrated embodiment, the electrode capacity of the high-frequency electrode 2 is Ci (i = 1 to 4), the capacity of the variable vacuum capacitor 4 is Ci '(i = 1 to 4), and the high-frequency electrode 2 is mounted. Assuming that the inductance of the copper connection base (not shown) is Li (i = 1 to 4), the impedance Zi (i = 1 to
4) is represented by Zi = jωLi + 1 / (Ci + Ci ′). Here, the capacitance Ci ′ (i = 1 to 4) of the variable vacuum capacitor 4 is set so that Z1 = Z2 = Z3 = Z4. As a result, high-frequency power is distributed uniformly over the entire high-frequency electrode 2.
【0013】次に、図示装置を用いてSiO2の基板
a、b、c、dをエッチングした実験例を示す。装置の
動作条件として真空チャンバー内にCF4とO2をそれ
ぞれ800SCCM、200SCCMづつ全部で1000SCCM流し、圧力を
10Paとし、基板と対向電極3との距離を110mmとし、投
入高周波電力を2.0kWとした条件Iの場合及び真空チャ
ンバーの圧力を7Paにし、他の条件は条件Iと同じにし
た条件IIの場合についてそれぞれ各基板におけるエッ
チング速度(オングストローム/分)を測定したところ
下記の結果が得られた。なお基板と対向電極3との距離
はガス、圧力及び放電周波数によって決定される。 基 板 条件Iの場合の 条件IIの場合の 電極内5点平均値 電極内5点平均値 a 661±8.2 643±3.1 b 652±7.1 654±4.1 c 668±8.6 638±2.5 d 659±6.3 648±1.8Next, an experimental example in which SiO 2 substrates a, b, c and d are etched using the illustrated apparatus will be described. As operating conditions of the apparatus, CF 4 and O 2 were flowed into the vacuum chamber at 800 SCCM and 200 SCCM, respectively, for a total of 1000 SCCM, and the pressure was increased
10 Pa, the distance between the substrate and the counter electrode 3 was 110 mm, the applied high frequency power was 2.0 kW, and the condition I was 2.0 kW, and the vacuum chamber pressure was 7 Pa, and the other conditions were the same as the condition I. When the etching rate (angstrom / min) of each substrate was measured, the following results were obtained. The distance between the substrate and the counter electrode 3 is determined by the gas, pressure, and discharge frequency. Substrate In case of condition I Average value of 5 points in electrode in case of condition II Average value of 5 points in electrode a 661 ± 8.2 643 ± 3.1 b 652 ± 7.1 654 ± 4.1 c 668 ± 8.6 638 ± 2.5 d 659 ± 6.3 648 ± 1.8
【0014】図2及び図3には、アノード電極を挟んで
両側に多数のカソード電極を設けた本発明の別の実施の
形態を示す。すなわち図示したように、長方形の真空チ
ャンバー1の下側壁とそれに対向した上側壁にはそれぞ
れカソード電極すなわち高周波電極2が四つずつ対称的
に設けられている。そして真空チャンバー1内において
上下両側の高周波電極2の中間位置すなわち真空チャン
バー1の長手方向中央軸線位置に沿って共通のアノード
電極3が配置されている。アノード電極3は図1に示す実
施の形態の場合と同様に接地されている。上下各側の高
周波電極2は二つずつ対を成してそれぞれの可変真空コ
ンデンサ4を介して共通のマッチング回路網5及び共通の
高周波電源6に接続されている。従って、八つの高周波
電極2に対してその半分の四つの高周波電源6が使用され
る。FIGS. 2 and 3 show another embodiment of the present invention in which a large number of cathode electrodes are provided on both sides of an anode electrode. That is, as shown, four cathode electrodes, that is, high-frequency electrodes 2 are provided symmetrically on the lower wall of the rectangular vacuum chamber 1 and on the upper wall opposed thereto, respectively. In the vacuum chamber 1, a common anode electrode 3 is arranged along an intermediate position between the upper and lower high-frequency electrodes 2, that is, along a longitudinal central axis of the vacuum chamber 1. The anode electrode 3 is grounded as in the embodiment shown in FIG. The upper and lower high-frequency electrodes 2 are paired two by two and connected to a common matching circuit network 5 and a common high-frequency power source 6 via respective variable vacuum capacitors 4. Therefore, four high-frequency power supplies 6 that are half of the eight high-frequency electrodes 2 are used.
【0015】また、各高周波電極2の両側と中央のアノ
ード電極3との間には図示したように、孔径が3mm以下
のパンチングメタルまたはメッシュメタルから成るアー
ス電位の仕切り部材7がそれぞれ設けられている。これ
らの仕切り部材7は、各高周波電極2と中央のアノード電
極3との間に画定された空間内に生成される放電プラズ
マを閉じこめる働きをすると共に、隣接高周波電極2間
の高周波干渉を抑制する。As shown in the figure, between the both sides of each high-frequency electrode 2 and the central anode electrode 3, partition members 7 having a ground potential made of a punching metal or mesh metal having a hole diameter of 3 mm or less are provided. I have. These partition members 7 function to confine the discharge plasma generated in the space defined between each high-frequency electrode 2 and the central anode electrode 3, and suppress high-frequency interference between adjacent high-frequency electrodes 2. .
【0016】図3には、図2の装置における一つの高周
波電極2とアノード電極3との関連構成の詳細を拡大して
示す。高周波電極2は真空チャンバー1の壁に設けた開口
部に例えばテフロン(登録商標)やアルミナから成る絶
縁部材8を介して真空密封的に取付けられている。また
高周波電極2は内部に水冷チャネル9を備えている。高
周波電極2の表面すなわちアノード電極3に対向した面
上にはアルミニウム製の台座10が固着手段11によって固
定され、その上に静電吸着電極12が設けられ、この静電
吸着電極12上に処理すべき基板、例えばフイルム状基板
(図示ていない)がアルミナ製のクランプ13によって装
着される。一般に、静電吸着電極12による吸着力は、処
理すべき基板の表面形状に依存し、使用される基板とし
ては吸着すべき導体に制限があり、しかもパターン形成
のためにレジストマスクを用いる表面に凸凹があるの
で、強くできない。また、基板の導体パターンでは強
く、それ以外の部分では弱い。さらに基板の熱膨張は材
質により異なり、基板の導体パターンでは熱膨張も大き
く、プラズマ処理中に膨みが発生し易い。この皺寄せが
基板の端面に生じると、基板の端部で異常放電が生じる
ことになる。また静電吸着電極12の表面材がプラズマで
エッチングされ、その結果寿命が短くなる。これらの課
題を解決するため、アルミナ製のクランプ13は、図示し
たように基板の周囲縁部を覆うように構成され、しかも
熱膨張を吸収するように構成され得る。さらに静電吸着
電極12にはリード線14を介して直流電源(図示していな
い)が接続され、この直流電源は好ましくは全てまたは
幾つかの静電吸着電極12に対して共通に設けられ得る。FIG. 3 is an enlarged view showing the details of the configuration of one high-frequency electrode 2 and one anode electrode 3 in the apparatus shown in FIG. The high-frequency electrode 2 is vacuum-sealed to an opening provided in the wall of the vacuum chamber 1 via an insulating member 8 made of, for example, Teflon (registered trademark) or alumina. The high-frequency electrode 2 has a water cooling channel 9 inside. A pedestal 10 made of aluminum is fixed on a surface of the high-frequency electrode 2, that is, a surface facing the anode electrode 3 by fixing means 11, and an electrostatic chucking electrode 12 is provided thereon. A substrate to be formed, for example, a film-like substrate (not shown) is mounted by a clamp 13 made of alumina. In general, the attraction force of the electrostatic attraction electrode 12 depends on the surface shape of the substrate to be processed, and the substrate to be used is limited in the conductor to be attracted. Because there are irregularities, it cannot be strengthened. Also, it is strong in the conductor pattern of the substrate and weak in other portions. Further, the thermal expansion of the substrate differs depending on the material. The thermal expansion is large in the conductor pattern of the substrate, and swelling is likely to occur during the plasma processing. When this wrinkling occurs on the end surface of the substrate, abnormal discharge occurs at the end of the substrate. Further, the surface material of the electrostatic attraction electrode 12 is etched by the plasma, so that the life is shortened. In order to solve these problems, the clamp 13 made of alumina may be configured to cover the peripheral edge of the substrate as shown in the figure, and may be configured to absorb thermal expansion. Further, a DC power supply (not shown) is connected to the electrostatic chucking electrode 12 via a lead wire 14, and this DC power supply can preferably be provided commonly to all or some of the electrostatic chucking electrodes 12. .
【0017】中央のアノード電極3は内部に水冷チャネ
ル15が設けられている。またアノード電極3と各高周波
電極2との間の空間において中央のアノード電極3寄り
にエッチングガス供給用ガスパイプ16が設けられてい
る。エッチングガスとしてはフッ素を含むハロゲンガス
とO2やN2の混合ガス、或いはこの混合ガスにさらに
CHF3などのCHを含むガスを混合したものなどが使
用され得る。The central anode electrode 3 has a water cooling channel 15 provided therein. An etching gas supply gas pipe 16 is provided near the center anode electrode 3 in the space between the anode electrode 3 and each high-frequency electrode 2. As the etching gas, a mixed gas of a halogen gas containing fluorine and O 2 or N 2 , or a mixed gas of this mixed gas and a gas containing CH such as CHF 3 can be used.
【0018】各高周波電極2の両側に設けら、プラズマ
領域を限定する仕切り部材7は、高周波プラズマによっ
て誘起される電位を最小にするために上述のようにアー
ス電位にされ、また各高周波電極2毎のガスの移動すな
わちガスの導入及び排気を容易にするため、仕切り部材
7は好ましくは開口率45%程度、しかもプラズマの漏れ
を抑制するため各孔の径3mm以下のメッシュやパンチン
グメタルで構成される。The partition members 7 provided on both sides of each high-frequency electrode 2 and defining a plasma region are set to the ground potential as described above in order to minimize the potential induced by the high-frequency plasma. The partitioning member 7 is preferably made of a mesh or punching metal having a diameter of 3 mm or less for each hole in order to facilitate the movement of the gas, that is, the introduction and exhaust of the gas, in order to facilitate the gas introduction and exhaust, and to suppress the plasma leakage. Is done.
【0019】ところで、図2及び図3に示す実施の形態
では、二つの高周波電極2に対して一つの高周波電源6
が用いられているが、必要により三つ以上の高周波電極
2を一つの高周波電源に接続するように構成することも
できる。また、図示装置はバッチ式の装置として実施し
ているが、当然ロードロック式の装置として実施するこ
とも可能である。さらに、本発明においては 上述のよ
うに、真空コンデンサに代えて、LC回路を使用しても同
様な作用効果を奏することができる。In the embodiment shown in FIGS. 2 and 3, one high-frequency power source 6 is connected to two high-frequency electrodes 2.
However, if necessary, three or more high-frequency electrodes 2 can be connected to one high-frequency power supply. Although the illustrated apparatus is implemented as a batch-type apparatus, the apparatus can be implemented as a load-lock-type apparatus. Further, in the present invention, as described above, the same operation and effect can be obtained by using an LC circuit instead of the vacuum capacitor.
【0020】以上説明してきたように、本発明によるプ
ラズマ処理装置においては、真空チャンバー内に設けら
れた複数の高周波電極のそれぞれに真空コンデンサまた
はLC回路を接続し、共通のマッチング回路網を介して共
通の高周波電源に接続するように構成しているので、全
高周波電極に高周波電力を均一に分配することができる
と共に、電源及びマッチング回路網の数を大幅に(実際
には半分以下に)削減することができるようになる。そ
の結果、装置のコストを大幅に低減させることができる
だけでなく、装置の重量も低減でき、さらにはメンテナ
ンスのための十分な空間が確保できるなどの効果が得ら
れる。As described above, in the plasma processing apparatus according to the present invention, a vacuum capacitor or an LC circuit is connected to each of a plurality of high-frequency electrodes provided in a vacuum chamber, and is connected via a common matching network. Since it is configured to be connected to a common high-frequency power supply, high-frequency power can be uniformly distributed to all high-frequency electrodes, and the number of power supplies and matching networks is significantly reduced (actually less than half). Will be able to As a result, not only can the cost of the apparatus be significantly reduced, but also the weight of the apparatus can be reduced, and further, an effect such as securing a sufficient space for maintenance can be obtained.
【図1】本発明の一つの実施の形態によるプラズマ処理
装置を示す概略線図。FIG. 1 is a schematic diagram showing a plasma processing apparatus according to one embodiment of the present invention.
【図2】本発明の別の実施の形態によるプラズマ処理装
置を示す概略線図。FIG. 2 is a schematic diagram showing a plasma processing apparatus according to another embodiment of the present invention.
【図3】図2に示すプラズマ処理装置の細部の構造を示
す拡大縦断面図。FIG. 3 is an enlarged vertical sectional view showing a detailed structure of the plasma processing apparatus shown in FIG. 2;
【図4】従来のプラズマ処理装置の一例を示す概略線
図。FIG. 4 is a schematic diagram illustrating an example of a conventional plasma processing apparatus.
1:真空チャンバー 2:高周波電極 3:アノード電極(対向電極) 4:真空コンデンサ 5:共通のマッチング回路網 6:共通の高周波電源 1: vacuum chamber 2: high-frequency electrode 3: anode electrode (counter electrode) 4: vacuum capacitor 5: common matching network 6: common high-frequency power supply
───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.7 識別記号 FI テーマコート゛(参考) H05H 1/46 H01L 21/302 C (72)発明者 太田 賀文 千葉県山武郡山武町横田523 日本真空技 術株式会社千葉超材料研究所内 (72)発明者 菊池 正志 神奈川県茅ケ崎市萩園2500番地 日本真空 技術株式会社内 (72)発明者 池田 均 神奈川県茅ケ崎市萩園2500番地 日本真空 技術株式会社内 (72)発明者 大園 雅 神奈川県茅ケ崎市萩園2500番地 日本真空 技術株式会社内 Fターム(参考) 4K030 FA03 KA14 4K057 DA20 DB11 DD01 DE06 DE08 DE14 DE20 DM02 DM40 5F004 AA16 BA06 BB13 BD04 CA02 CA03 DA01 DA25 DA26 5F045 AA08 AC11 AC15 BB08 EH04 EH06 EH13 ──────────────────────────────────────────────────続 き Continued on the front page (51) Int.Cl. 7 Identification symbol FI Theme coat ゛ (Reference) H05H 1/46 H01L 21/302 C (72) Inventor Kafumi Ota 523 Yokota, Sanmu-cho, Sanmu-gun, Chiba Nihon Vacuum (72) Inventor Masashi Kikuchi 2500 Hagizono, Chigasaki-shi, Kanagawa Japan Vacuum Engineering Co., Ltd. (72) Inventor Hitoshi Ikeda 2500 Hagizono, Chigasaki-shi, Kanagawa Japan Vacuum Engineering Co., Ltd. 72) Inventor Masaru Ozono 2500 Hagizono, Chigasaki-shi, Kanagawa Japan F-term (reference) 4K030 FA03 KA14 4K057 DA20 DB11 DD01 DE06 DE08 DE14 DE20 DM02 DM40 5F004 AA16 BA06 BB13 BD04 CA02 CA03 DA01 DA25 DA26 5F045 AA08 AC11 AC15 BB08 EH04 EH06 EH13
Claims (5)
の高周波電極のそれぞれに処理すべき基板を装着し、真
空チャンバー内に発生されたプラズマを利用して所定の
処理を行うようにしたプラズマ処理装置において、 真空チャンバー内に設けられた複数の高周波電極をそれ
ぞれの真空コンデンサ及び共通のマッチング回路網を介
して共通の高周波電源に接続したことを特徴とするプラ
ズマ処理装置。1. A plasma in which a substrate to be processed is mounted on each of a plurality of high-frequency electrodes provided in one vacuum chamber, and a predetermined process is performed using plasma generated in the vacuum chamber. A plasma processing apparatus, wherein a plurality of high-frequency electrodes provided in a vacuum chamber are connected to a common high-frequency power supply via respective vacuum capacitors and a common matching network.
波電極を複数のグループに分け、各グループにおける複
数の高周波電極をそれぞれの真空コンデンサ及び共通の
マッチング回路網を介して共通の高周波電源に接続した
ことを特徴とする請求項1に記載のプラズマ処理装置。2. A plurality of high-frequency electrodes provided in a vacuum chamber are divided into a plurality of groups, and the plurality of high-frequency electrodes in each group are connected to a common high-frequency power supply via respective vacuum capacitors and a common matching network. The plasma processing apparatus according to claim 1, wherein:
が可変真空コンデンサであることを特徴とする請求項1
または2に記載のプラズマ処理装置。3. The vacuum capacitor connected to each high-frequency electrode is a variable vacuum capacitor.
Or the plasma processing apparatus according to 2.
の高周波電極のそれぞれに処理すべき基板を装着し、真
空チャンバー内に発生されたプラズマを利用して所定の
処理を行うようにしたプラズマ処理装置において、 真空チャンバー内に設けられた複数の高周波電極をそれ
ぞれのLC回路及び共通のマッチング回路網を介して共通
の高周波電源に接続したことを特徴とするプラズマ処理
装置。4. A plasma in which a substrate to be processed is mounted on each of a plurality of high-frequency electrodes provided in one vacuum chamber, and a predetermined process is performed using plasma generated in the vacuum chamber. A plasma processing apparatus, wherein a plurality of high-frequency electrodes provided in a vacuum chamber are connected to a common high-frequency power supply via respective LC circuits and a common matching network.
波電極を複数のグループに分け、各グループにおける複
数の高周波電極をそれぞれのLC回路及び共通のマッチン
グ回路網を介して共通の高周波電源に接続したことを特
徴とする請求項4に記載のプラズマ処理装置。5. A plurality of high-frequency electrodes provided in a vacuum chamber are divided into a plurality of groups, and the plurality of high-frequency electrodes in each group are connected to a common high-frequency power supply via respective LC circuits and a common matching network. The plasma processing apparatus according to claim 4, wherein:
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JP2009231247A (en) * | 2008-03-25 | 2009-10-08 | Tokyo Electron Ltd | Plasma treatment device, and supplying method of high frequency power |
US20110297320A1 (en) * | 2010-06-02 | 2011-12-08 | Hitachi High-Technologies Corporation | Plasma processing apparatus |
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CN108630511A (en) * | 2017-03-17 | 2018-10-09 | 北京北方华创微电子装备有限公司 | Lower electrode device and semiconductor processing equipment |
JP2020066764A (en) * | 2018-10-23 | 2020-04-30 | 東京エレクトロン株式会社 | Film formation device and film formation method |
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JP2020066764A (en) * | 2018-10-23 | 2020-04-30 | 東京エレクトロン株式会社 | Film formation device and film formation method |
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