JP2002208587A - Plasma processing method and apparatus - Google Patents
Plasma processing method and apparatusInfo
- Publication number
- JP2002208587A JP2002208587A JP2001004371A JP2001004371A JP2002208587A JP 2002208587 A JP2002208587 A JP 2002208587A JP 2001004371 A JP2001004371 A JP 2001004371A JP 2001004371 A JP2001004371 A JP 2001004371A JP 2002208587 A JP2002208587 A JP 2002208587A
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- Prior art keywords
- plasma
- processing chamber
- processed
- electrode
- substrate electrode
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- Physical Or Chemical Processes And Apparatus (AREA)
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- Drying Of Semiconductors (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明はプラズマ処理方法お
よび装置に係り、特にプラズマを用いて半導体等の被処
理材の表面処理を行うのに好適なプラズマ処理方法およ
び装置に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a plasma processing method and apparatus, and more particularly to a plasma processing method and apparatus suitable for performing surface treatment of a material to be processed such as a semiconductor using plasma.
【0002】[0002]
【従来の技術】エッチング処理を行うプラズマ処理装置
の場合、処理ガスを効率よく電離し活性化することで処
理の高速化を図り、また被処理材に高周波バイアス電力
を供給しプラズマ中のイオンを被処理材に対して垂直に
入射させることで、異方性を向上させ高精度なエッチン
グ処理を実現している。このような処理を行うプラズマ
処理装置としては、例えば、特開平9−321031号
公報に記載されているような有磁場UHF帯のエッチン
グ装置が知られている。2. Description of the Related Art In the case of a plasma processing apparatus for performing an etching process, a process gas is efficiently ionized and activated to speed up the process, and a high-frequency bias power is supplied to a material to be processed to remove ions in the plasma. By making the light perpendicularly incident on the material to be processed, anisotropy is improved and highly accurate etching processing is realized. As a plasma processing apparatus for performing such a process, for example, an etching apparatus in a magnetic field UHF band as described in Japanese Patent Application Laid-Open No. 9-321031 is known.
【0003】有磁場UHF帯のエッチング装置は、真空
容器内で被加工試料に対面する位置に円形導体板を配置
し、円形導体板にUHF帯の電磁波を供給するとともに
真空容器内に磁場を形成してECRプラズマを発生さ
せ、UHF帯とは異なる周波数の電界を円形導体板に重
畳し、円形導体板にかかるバイアスを大きくして円形導
体板と反応ガスとの反応性を高めて、エッチング反応に
寄与する活性種を多く生成させるとともに、被加工試料
が配置される試料台にバイアス電圧を印加して被加工試
料をプラズマ処理している。なお、この装置は、試料台
に印加する高周波電源と、試料台に対向する円形導体板
に印加するUHF帯の高周波電源と、同じ円形導体板に
印加するUHF帯高周波電源とは異なる高周波電源とを
独立に制御することができるようになっている。In a magnetic field UHF band etching apparatus, a circular conductor plate is arranged at a position facing a sample to be processed in a vacuum vessel, an electromagnetic wave in the UHF band is supplied to the circular conductor plate, and a magnetic field is formed in the vacuum vessel. ECR plasma is generated, an electric field having a frequency different from that of the UHF band is superimposed on the circular conductor plate, the bias applied to the circular conductor plate is increased, the reactivity between the circular conductor plate and the reaction gas is increased, and the etching reaction is performed. In addition to generating a large number of active species contributing to the sample, a bias voltage is applied to the sample stage on which the sample to be processed is arranged, and the sample to be processed is plasma-processed. The apparatus includes a high-frequency power source applied to the sample stage, a UHF-band high-frequency power source applied to a circular conductor plate facing the sample stage, and a high-frequency power source different from the UHF-band high-frequency power source applied to the same circular conductor plate. Can be controlled independently.
【0004】また、このような有磁場プラズマ処理装置
内では、リアライズ社1996発行「半導体プロセスに
おけるチャージングダメージ」中村守孝編、P.9〜2
8 記載のように、磁場に対して垂直方向のプラズマイ
ンピーダンスが平行方向のプラズマインピーダンスに比
べて大きくなり、被処理材面内に電位分布を形成する可
能性があることが知られていた。In such a magnetic field plasma processing apparatus, "Charging Damage in Semiconductor Process" published by Realize Inc., 1996, edited by Moritaka Nakamura, pp. 9-2.
As described in 8, it has been known that the plasma impedance in the direction perpendicular to the magnetic field becomes larger than the plasma impedance in the direction parallel to the magnetic field, and there is a possibility of forming a potential distribution in the surface of the material to be processed.
【0005】[0005]
【発明が解決しようとする課題】半導体集積回路の集積
度が高まりつつある現在、例えば、半導体素子の代表的
な一例であるMOS(Metal Oxide Semiconductor)トラ
ンジスタゲート酸化膜等の薄膜化が進み、ゲート酸化膜
の加工において、プラズマ処理時にゲート酸化膜が絶縁
破壊する(チャージングダメージ)問題が深刻になりつ
つある。上記従来技術におけるプラズマ処理装置では、
被処理材に印加された高周波電力による電界が試料台と
接地電位にある真空容器側面との間に形成され、高周波
電力が磁場を横切る方向に伝播する。このため、被処理
材面内に電位分布が形成され、ゲート酸化膜の耐電圧を
劣化させるチャージングダメージを発生させる恐れがあ
る。At present, as the degree of integration of a semiconductor integrated circuit is increasing, for example, a MOS (Metal Oxide Semiconductor) transistor, which is a typical example of a semiconductor device, is becoming thinner, and the gate is becoming thinner. In the processing of an oxide film, the problem of dielectric breakdown (charging damage) of a gate oxide film during plasma processing is becoming more serious. In the above-described plasma processing apparatus in the related art,
An electric field due to the high-frequency power applied to the material to be processed is formed between the sample stage and the side of the vacuum vessel at the ground potential, and the high-frequency power propagates in a direction crossing the magnetic field. For this reason, a potential distribution is formed in the surface of the material to be processed, and there is a possibility that charging damage that deteriorates the withstand voltage of the gate oxide film may occur.
【0006】本発明の目的は、チャージングダメージを
抑制し、半導体デバイスの歩留まりを高め、高精度な表
面処理を行なうことのできるプラズマ処理方法および装
置を提供することにある。An object of the present invention is to provide a plasma processing method and apparatus capable of suppressing charging damage, increasing the yield of semiconductor devices, and performing highly accurate surface treatment.
【0007】[0007]
【課題を解決するための手段】上記目的は、真空排気装
置が接続され内部を減圧可能な処理室と、処理室内へガ
スを供給するガス供給装置と、処理室内に設けられ被処
理材を載置可能な基板電極と、処理室内に供給されたガ
スをプラズマ化する電磁波を処理室内に放射する第1の
高周波電源と、基板電極へ接続され被処理材に基板バイ
アス電圧を印加する第2の高周波電源とを具備し、基板
電極に印加する高周波電圧の正のピーク電圧に対し、そ
の値より大きい正のピーク電圧が発生する補助電極を被
処理材の外周部に設けた装置とし、処理ガスが供給され
内部が所定圧力に減圧排気された処理室内にプラズマを
生成するとともに、処理室内に設けられた基板電極にバ
イアス電圧を印加し、プラズマの生成とは独立にプラズ
マ中のイオンの被処理材への入射エネルギを制御し、被
処理材を処理する際に、基板電極外周部のプラズマ電位
を被処理材上のプラズマ電位よりも高くして処理する方
法とすることにより、達成される。SUMMARY OF THE INVENTION The object of the present invention is to provide a processing chamber to which a vacuum exhaust device is connected and whose inside can be depressurized, a gas supply device for supplying gas into the processing chamber, and a processing chamber provided in the processing chamber. A substrate electrode that can be mounted, a first high-frequency power supply that emits an electromagnetic wave that converts a gas supplied into the processing chamber into plasma into the processing chamber, and a second high-frequency power supply that is connected to the substrate electrode and applies a substrate bias voltage to a material to be processed. A high-frequency power supply, and an apparatus in which an auxiliary electrode that generates a positive peak voltage greater than the positive peak voltage of the high-frequency voltage applied to the substrate electrode is provided on the outer peripheral portion of the material to be processed, and the processing gas Is supplied to the inside of the processing chamber, the inside of which is evacuated to a predetermined pressure, and a bias voltage is applied to a substrate electrode provided in the processing chamber, so that ions in the plasma are exposed independently of the generation of the plasma. This is achieved by controlling the incident energy to the processing material and processing the material to be processed by setting the plasma potential at the outer peripheral portion of the substrate electrode higher than the plasma potential on the material to be processed. .
【0008】すなわち、電極外周部のプラズマ電位を高
くすることで、電位の高い被処理材面内から電位の低い
(接地電位の)処理室内壁面、すなわち、処理室を形成
する真空容器の内壁側面に形成されようとする回路の形
成が阻害されるので、被処理材面内に生じる電位差を低
減することができる。これにより、プラズマ特性の面内
分布に起因する被処理材面内の電位分布を均一にするこ
とができる。さらに、処理室内に基板電極と対向するア
ンテナ電極を設けた場合、基板電極に高周波電圧を印加
しても、基板電極外周部のプラズマ電位が高いため、基
板電極からアースとして機能する処理室内壁への電流の
流れは減少し、対向アース電極として機能するアンテナ
電極との間での電流が増加する。すなわち、高周波電流
が処理室内壁よりも対向する電極間でより多く流れるよ
うになるので、磁場を横切る方向の電流が減少し、磁場
に対して垂直方向のプラズマインピーダンスの影響を受
けなくなる。磁場に対して水平方向のプラズマインピー
ダンスは面内で均一なので、プラズマ特性の面内分布に
起因する被処理材面内の電位分布はさらに低減され、チ
ャージングダメージ発生を抑制することができ、高精度
なプラズマ処理が可能となる。That is, by increasing the plasma potential at the outer peripheral portion of the electrode, the inside of the processing chamber having a low potential (ground potential), that is, the side wall of the inner wall of the vacuum vessel forming the processing chamber is changed from the surface of the material to be processed having a high potential. Since the formation of the circuit to be formed is inhibited, the potential difference generated in the surface of the material to be processed can be reduced. Thus, the potential distribution in the surface of the material to be processed due to the in-plane distribution of the plasma characteristics can be made uniform. Further, in the case where an antenna electrode facing the substrate electrode is provided in the processing chamber, even if a high-frequency voltage is applied to the substrate electrode, the plasma potential at the outer peripheral portion of the substrate electrode is high, so that the substrate electrode is transferred to the processing chamber wall functioning as an earth. , The current flowing between the antenna electrode and the antenna electrode functioning as the opposite ground electrode increases. That is, since the high-frequency current flows more between the electrodes facing each other than the inner wall of the processing chamber, the current in the direction crossing the magnetic field decreases, and the magnetic field is not affected by the plasma impedance in the direction perpendicular to the magnetic field. Since the plasma impedance in the horizontal direction to the magnetic field is uniform in the plane, the potential distribution in the surface of the workpiece due to the in-plane distribution of the plasma characteristics is further reduced, and the occurrence of charging damage can be suppressed. Accurate plasma processing becomes possible.
【0009】また、アンテナ電極に第3の高周波電源を
接続し、基板電極に接続された第1の高周波電源とアン
テナ電極に接続された第3の高周波電源の周波数を同一
周波数とする装置とし、それぞれの高周波電源の位相差
を180°±30°とすることで、基板電極の正の高周
波ピーク電圧を小さくすることができ、被処理材上のプ
ラズマ電位からみた基板電極外周部のプラズマ電位をさ
らに高くすることができる。これにより、対向する電極
が効率よくアースとして機能する効果をさらに増幅し、
チャージングダメージ発生を抑制することができ、高精
度なプラズマ処理が可能となる。A third high-frequency power supply is connected to the antenna electrode, and the frequency of the first high-frequency power supply connected to the substrate electrode and the third high-frequency power supply connected to the antenna electrode are set to be the same frequency. By setting the phase difference of each high-frequency power supply to 180 ° ± 30 °, the positive high-frequency peak voltage of the substrate electrode can be reduced, and the plasma potential of the outer peripheral portion of the substrate electrode as viewed from the plasma potential on the workpiece is reduced. It can be even higher. This further amplifies the effect of the opposing electrode functioning efficiently as ground,
The occurrence of charging damage can be suppressed, and highly accurate plasma processing can be performed.
【0010】[0010]
【発明の実施の形態】[実施例1]以下、本発明の第1
の実施例を図1から図3を用いて説明する。図1は、本
発明を適用するプラズマ処理装置の一実施例であるエッ
チング装置の縦断面図である。上部が開放された真空容
器101の上部に処理容器104,誘電体窓102(例
えば石英製),アンテナ電極103(例えばSi製)を
設置、アンテナカバー121で密封することにより処理
室105を形成する。処理室104の外周部とアンテナ
カバー121上部には磁場発生用コイル114が設置さ
れている。アンテナ電極103はエッチングガスを流す
ための多孔構造となっておりガス供給装置107に接続
されている。また真空容器101には真空排気口106
を介して真空排気装置(図示省略)が接続されている。[Embodiment 1] Hereinafter, the first embodiment of the present invention will be described.
The embodiment will be described with reference to FIGS. FIG. 1 is a longitudinal sectional view of an etching apparatus which is an embodiment of a plasma processing apparatus to which the present invention is applied. A processing chamber 104, a dielectric window 102 (for example, made of quartz), and an antenna electrode 103 (for example, made of Si) are installed on the upper part of a vacuum vessel 101 having an open top, and a processing chamber 105 is formed by sealing with an antenna cover 121. . A magnetic field generating coil 114 is provided on the outer peripheral portion of the processing chamber 104 and on the antenna cover 121. The antenna electrode 103 has a porous structure for flowing an etching gas, and is connected to a gas supply device 107. The vacuum container 101 has a vacuum exhaust port 106.
Is connected to a vacuum exhaust device (not shown).
【0011】アンテナ電極103上部には同軸線路11
1,整合器110,フィルタ109を介して高周波電源
108(例えば周波数450MHz)がプラズマ生成用
電源として接続されている。さらに、アンテナ電極10
3上部には同軸線路111,整合器119,フィルタ1
13を介してアンテナバイアス電源112(例えば周波
数13.56MHz )が接続されている。また、被処理
材116を載置可能な基板電極115は真空容器101
下部に設置され、同軸線路122,整合器118を介して
基板バイアス電源117(例えば周波数800KHz)
に接続されている。高周波電源108によりプラズマを
生成し、アンテナバイアス電源112によりプラズマ組
成あるいはプラズマ分布を制御し、基板バイアス電源1
17により基板への入射イオン量を制御している。この
ような構成により、プラズマ生成、プラズマ組成・分
布、被処理材116への入射イオン量を独立に制御でき
るという利点がある。また被処理材116を静電的に吸
着させるために静電チャック電源120が基板電極11
5に接続されている。The coaxial line 11 is provided above the antenna electrode 103.
1, a high-frequency power supply 108 (for example, a frequency of 450 MHz) is connected as a power supply for plasma generation via a matching unit 110 and a filter 109. Further, the antenna electrode 10
3, a coaxial line 111, a matching unit 119, and a filter 1
An antenna bias power supply 112 (for example, a frequency of 13.56 MHz) is connected via the power supply 13. The substrate electrode 115 on which the material to be processed 116 can be placed is the vacuum vessel 101.
A substrate bias power supply 117 (e.g., a frequency of 800 KHz) is provided at a lower portion and passes through a coaxial line 122 and a matching unit 118.
It is connected to the. Plasma is generated by the high-frequency power supply 108, and the plasma composition or plasma distribution is controlled by the antenna bias power supply 112.
Reference numeral 17 controls the amount of ions incident on the substrate. With such a configuration, there is an advantage that the plasma generation, the plasma composition / distribution, and the amount of ions incident on the processing target material 116 can be independently controlled. Further, in order to electrostatically attract the processing target material 116, the electrostatic chuck power supply 120 is connected to the substrate electrode 11.
5 is connected.
【0012】基板電極115の外周部に補助電極127
を設置しており、補助電極127は電位制御回路12
6,同軸線路122を介して整合器118に接続されて
いる。An auxiliary electrode 127 is provided on the outer periphery of the substrate electrode 115.
And the auxiliary electrode 127 is connected to the potential control circuit 12.
6, connected to the matching unit 118 via the coaxial line 122.
【0013】図2に電位制御回路126の回路構成例を
示す。電位制御回路126は基板バイアス電源117か
らの高周波電圧の波形を任意の電圧波形に制御する回路
である。補助電極127と同軸線路122の間に、コン
デンサ(C1)およびダイオード(D1)を並列に接続
する。ダイオード(D1)は補助電極から同軸線路12
2へ向う方向を順方向になるよう接続する。基板バイア
ス電源117により高周波電圧が補助電極127に印加
されたとき、前記回路構成により、プラズマ中からの補
助電極127への電子の流入を抑制し、補助電極127
の高周波自己バイアス電圧(Vdc)の絶対値を小さく
するように作用させる。FIG. 2 shows a circuit configuration example of the potential control circuit 126. The potential control circuit 126 is a circuit that controls the waveform of the high-frequency voltage from the substrate bias power supply 117 to an arbitrary voltage waveform. A capacitor (C1) and a diode (D1) are connected in parallel between the auxiliary electrode 127 and the coaxial line 122. The diode (D1) is connected to the coaxial line 12 from the auxiliary electrode.
Connect so that the direction toward 2 is forward. When a high-frequency voltage is applied to the auxiliary electrode 127 by the substrate bias power supply 117, the circuit configuration suppresses the flow of electrons from the plasma to the auxiliary electrode 127, and the auxiliary electrode 127
To reduce the absolute value of the high frequency self-bias voltage (Vdc).
【0014】上記のように構成された装置において、処
理室105内部を真空排気装置により減圧した後、ガス
供給装置107によりエッチングガスを処理室105内
に導入し所望の圧力に調整する。高周波電源108より
発振された、例えば、周波数450MHzの高周波電力
は同軸線路111を伝播し、アンテナ電極103および
誘電体窓102を介して処理室105内に導入され、磁
場発生用コイル114(例えば、ソレノイドコイル)に
より形成された磁場との相互作用により、処理室105
内に高密度プラズマを生成する。特に電子サイクロトロ
ン共鳴を起こす磁場強度(例えば、160G)を処理室
内に形成した場合、効率良く高密度プラズマを生成する
ことができる。また、アンテナバイアス電源112より
高周波電力(例えば、周波数13.56MHz)が同軸
線路111を介してアンテナ電極103に供給される。
また基板電極115に載置された被処理材116は、基
板バイアス電源117より高周波電力(例えば、周波数
800KHz)が供給され、表面処理(例えば、エッチ
ング処理)される。In the apparatus configured as described above, after the inside of the processing chamber 105 is depressurized by the vacuum exhaust device, the etching gas is introduced into the processing chamber 105 by the gas supply device 107 and adjusted to a desired pressure. High-frequency power having a frequency of, for example, 450 MHz, oscillated from the high-frequency power supply 108, propagates through the coaxial line 111, is introduced into the processing chamber 105 through the antenna electrode 103 and the dielectric window 102, and is provided with a magnetic field generating coil 114 (for example, The processing chamber 105 interacts with the magnetic field formed by the solenoid coil.
A high-density plasma is generated inside. In particular, when a magnetic field strength (for example, 160 G) that causes electron cyclotron resonance is formed in the processing chamber, high-density plasma can be efficiently generated. Further, high frequency power (for example, frequency of 13.56 MHz) is supplied from the antenna bias power supply 112 to the antenna electrode 103 via the coaxial line 111.
The workpiece 116 placed on the substrate electrode 115 is supplied with high-frequency power (for example, a frequency of 800 KHz) from the substrate bias power supply 117 and subjected to a surface treatment (for example, an etching process).
【0015】基板電極115には、例えば、ピーク・ツ
ウ・ピーク電圧(Vpp)800Vの高周波電力が供給
され、自己バイアス電圧(Vdc)が発生し、基板電極1
15の正の高周波ピーク電圧は100V〜200V程度
に固定される。このとき、補助電極127にも高周波が
印加されるが、ダイオード(D1)が順方向に接続され
るとともに整合器118内のコンデンサよりも容量の小
さいコンデンサ(C1)を並列に設けているため、高周波
電圧の正電圧が補助電極に印加された際、ダイオード
(D1)によりプラズマ中から引き寄せられる電子は整
合器118側へは流れることができず、またコンデンサ
(C1)の容量が小さいため補助電極127に蓄積される
電子量も少なくなり、補助電極127における自己バイ
アス電圧(Vdc)の絶対値は小さい値となる。電子電
流が抑制され、自己バイアス電圧(Vdc)の絶対値が
小さくなるため補助電極127の正の高周波ピーク電圧
は基板電極115より高くなり、基板電極115上のプ
ラズマ電位より、補助電極127上のプラズマ電位が高
くなる。図3に補助電極127に高周波電圧を印加した
ときのプラズマ電位状態を示す。補助電極127上のプ
ラズマ電位が高くなることで、被処理材116面内の電
位分布は低減され、プラズマ特性の面内分布を均一にす
ることができる。さらに、基板電極115と処理室10
5の側壁である処理容器104との間にプラズマを介し
て形成される回路には途中に高いプラズマ電位が存在す
るので該回路に流れる電流が減少し、高周波電流が側壁
よりも対向する電極間にさらに多く流れるようになる。
これにより、磁場を横切る方向の電流が減少しチャージ
ングダメージの発生が抑制され、さらに高精度エッチン
グ処理ができるという効果がある。 [実施例2]本発明の第2の実施例を図4を用いて説明
する。本図において図1と同符号は同一部材を示し説明
を省略する。本図が図1と異なる点を以下に説明する。
アンテナ電極103上部には同軸線路111,整合器1
19,フィルタ113を介してアンテナバイアス電源1
12(例えば、周波数800KHz)が接続されてい
る。また、被処理材116を載置可能な基板電極115
は真空容器101下部に設置され、同軸線路122,整
合器118を介して基板バイアス電源117(例えば、
周波数800KHz)に接続されている。アンテナバイ
アス電源112と基板バイアス電源117は位相制御器
125に接続されており、アンテナバイアス電源112
と基板バイアス電源117より出力される高周波の位相
を制御することができる。ここではアンテナバイアス電
源112と基板バイアス電源117の周波数は同一周波
数としてある。A high frequency power of, for example, 800 V peak-to-peak voltage (Vpp) is supplied to the substrate electrode 115 to generate a self-bias voltage (Vdc).
The 15 positive high-frequency peak voltages are fixed at about 100V to 200V. At this time, a high frequency is also applied to the auxiliary electrode 127, but since the diode (D1) is connected in the forward direction and the capacitor (C1) having a smaller capacity than the capacitor in the matching unit 118 is provided in parallel, When a positive voltage of a high-frequency voltage is applied to the auxiliary electrode, electrons attracted from the plasma by the diode (D1) cannot flow toward the matching unit 118, and
Since the capacitance of (C1) is small, the amount of electrons stored in the auxiliary electrode 127 is also small, and the absolute value of the self-bias voltage (Vdc) at the auxiliary electrode 127 is small. Since the electron current is suppressed and the absolute value of the self-bias voltage (Vdc) becomes smaller, the positive high-frequency peak voltage of the auxiliary electrode 127 becomes higher than that of the substrate electrode 115, and the plasma potential on the auxiliary electrode 127 becomes higher than the plasma potential on the substrate electrode 115. The plasma potential increases. FIG. 3 shows a plasma potential state when a high-frequency voltage is applied to the auxiliary electrode 127. By increasing the plasma potential on the auxiliary electrode 127, the potential distribution in the surface of the processing target material 116 is reduced, and the in-plane distribution of plasma characteristics can be made uniform. Furthermore, the substrate electrode 115 and the processing chamber 10
5 has a high plasma potential in the middle of the circuit formed between the processing container 104 and the processing container 104, and the current flowing through the circuit is reduced. More will be flowing.
As a result, there is an effect that the current in the direction crossing the magnetic field decreases, the occurrence of charging damage is suppressed, and a highly accurate etching process can be performed. Embodiment 2 A second embodiment of the present invention will be described with reference to FIG. In this figure, the same reference numerals as those in FIG. 1 denote the same members, and a description thereof will be omitted. The difference between this figure and FIG. 1 will be described below.
A coaxial line 111 and a matching device 1 are provided above the antenna electrode 103.
19. Antenna bias power supply 1 via filter 113
12 (for example, frequency 800 KHz) are connected. Further, a substrate electrode 115 on which the processing target material 116 can be placed
Is installed below the vacuum vessel 101, and a substrate bias power supply 117 (for example,
(Frequency 800 KHz). The antenna bias power supply 112 and the substrate bias power supply 117 are connected to the phase controller 125, and the antenna bias power supply 112
And the phase of the high frequency output from the substrate bias power supply 117 can be controlled. Here, the frequencies of the antenna bias power supply 112 and the substrate bias power supply 117 are the same.
【0016】アンテナ電極103と基板電極115に印
加される高周波電圧の位相差が180°±30°の場
合、例えば、基板電極115に正の電圧が印加されてい
るとき、アンテナ電極103には負の電圧が印加される
ので、アンテナ電極103にはイオンが入射するが電子
は入射せず、アンテナ電極103近傍は電子が多く存在
する状態となり、対向する電極が効率よくアースとして
の機能を有する。位相差180°±30°で印加するこ
とで、基板電極115から対向するアースとなるアンテ
ナ電極103までのインピーダンスは低減され、例え
ば、ピーク・ツウ・ピーク電圧(Vpp)800Vの高
周波電力が印加されると基板電極115の正の高周波ピ
ーク電圧は20〜30Vに固定される。実施例1で示し
た基板電極115の正の高周波ピーク電圧より本実施例
の基板電極115の正の高周波ピーク電圧が小さくな
り、対向する電極が効率よくアースとして機能する効果
をさらに増幅して実現することが可能となる。基板電極
115上のプラズマ電位からみた補助電極127上のプ
ラズマ電位をさらに高くすることで、高周波電流が側壁
よりも対向する電極間にさらに多く流れることから、磁
場を横切る方向の電流が減少しチャージングダメージの
発生を抑制でき、高精度エッチング処理ができるという
効果がある。 [実施例3]本発明の第3の実施例を図5を用いて説明
する。本図において図2と同符号は同一部材を示し説明
を省略する。本図が図2と異なる点を以下に説明する。
電位制御回路126のダイオード(D1)を図2と逆方
向に接続し、可変抵抗器R1を直列に追加接続した点、
電位制御回路126のコンデンサ(C1)を可変容量コ
ンデンサとした点、可変抵抗器R1の抵抗値と可変容量
コンデンサC1の容量を調整するための制御装置128
を接続している点である。When the phase difference between the high-frequency voltages applied to the antenna electrode 103 and the substrate electrode 115 is 180 ° ± 30 °, for example, when a positive voltage is applied to the substrate electrode 115, the antenna electrode 103 becomes negative. Is applied, ions are incident on the antenna electrode 103 but no electrons are incident on the antenna electrode 103, and a lot of electrons are present in the vicinity of the antenna electrode 103, and the opposing electrode has a function as a ground efficiently. When the phase difference is applied at 180 ° ± 30 °, the impedance from the substrate electrode 115 to the opposing grounding antenna electrode 103 is reduced. For example, a high-frequency power of 800V peak-to-peak voltage (Vpp) is applied. Then, the positive high frequency peak voltage of the substrate electrode 115 is fixed at 20 to 30V. The positive high-frequency peak voltage of the substrate electrode 115 of this embodiment is smaller than the positive high-frequency peak voltage of the substrate electrode 115 shown in the first embodiment, and the effect that the opposing electrode efficiently functions as ground is further amplified and realized. It is possible to do. By further increasing the plasma potential on the auxiliary electrode 127 from the viewpoint of the plasma potential on the substrate electrode 115, more high-frequency current flows between the electrodes facing each other than the side wall, so that the current in the direction crossing the magnetic field decreases and the charge increases. This has the effect of suppressing the occurrence of etching damage and enabling high-precision etching. [Embodiment 3] A third embodiment of the present invention will be described with reference to FIG. 2, the same reference numerals as those in FIG. 2 denote the same members, and a description thereof will be omitted. The difference between this figure and FIG. 2 will be described below.
A point that the diode (D1) of the potential control circuit 126 is connected in the opposite direction to that of FIG. 2 and the variable resistor R1 is additionally connected in series;
A point that the capacitor (C1) of the potential control circuit 126 is a variable capacitor, and a controller 128 for adjusting the resistance value of the variable resistor R1 and the capacity of the variable capacitor C1.
Is connected.
【0017】このような構成により、基板バイアス電源
117により高周波電圧が補助電極127に印加された
ときに、例えば、抵抗R1の抵抗値を大きくして電流の
流れを抑制することでプラズマ中からの補助電極127
への電子の流入を抑制でき、また抵抗R1の抵抗値を小
さくして電流を流れ易くすることでプラズマ中からの補
助電極127への電子の流入を多くすることができる。
これにより、補助電極127の高周波自己バイアス電圧
(Vdc)の絶対値を制御できるので、自己バイアス電
圧(Vdc)が小さくなるように作用させ、前記実施例
1と同様に補助電極127上でのプラズマ電位を高くし
たり、自己バイアス電圧(Vdc)を少し大きくしてプラ
ズマ中のイオンが補助電極127に入射されるように
し、イオンの入射量を制御できるようにする。補助電極
127へのイオンの入射によって、補助電極127表面
でのプラズマ中の活性種との反応を制御することも可能
である。例えば、CF系のガスを用いた酸化膜エッチン
グにおいて、補助電極127の材質を高純度のシリコン
とすれば、シリコンのスカベンジ作用により補助電極1
27でのFラジカルやCFラジカルの反応を制御して、
特にウェハ外周部でのエッチング均一性を向上させるこ
とができる。With this configuration, when a high-frequency voltage is applied to the auxiliary electrode 127 by the substrate bias power supply 117, for example, the resistance value of the resistor R1 is increased to suppress the flow of current, thereby reducing the current flow from the plasma. Auxiliary electrode 127
The flow of electrons into the auxiliary electrode 127 from the plasma can be increased by reducing the resistance value of the resistor R1 and making the current easier to flow.
Thus, the absolute value of the high-frequency self-bias voltage (Vdc) of the auxiliary electrode 127 can be controlled, so that the self-bias voltage (Vdc) is reduced, and the plasma on the auxiliary electrode 127 is actuated as in the first embodiment. The potential in the plasma is increased or the self-bias voltage (Vdc) is slightly increased so that the ions in the plasma are incident on the auxiliary electrode 127 so that the incident amount of the ions can be controlled. It is also possible to control the reaction with the active species in the plasma on the surface of the auxiliary electrode 127 by the incidence of ions on the auxiliary electrode 127. For example, in the oxide film etching using a CF-based gas, if the material of the auxiliary electrode 127 is made of high-purity silicon, the auxiliary electrode 1 is formed by a scavenging action of silicon.
By controlling the reaction of F radicals and CF radicals at 27,
In particular, it is possible to improve the etching uniformity in the outer peripheral portion of the wafer.
【0018】また、基板バイアス電源117により高周
波電圧が補助電極127に印加されたときに、例えば、
コンデンサC1の容量を小さくして印加する高周波電力
を抑制することでプラズマ中からの補助電極127への
イオンの流入を抑制でき、またコンデンサC1の容量を
大きくして印加する高周波電力を増加させることでプラ
ズマ中からの補助電極127へのイオンの流入を多くす
ることができる。これにより、補助電極127の高周波
自己バイアス電圧(Vdc)の絶対値を制御できるの
で、自己バイアス電圧(Vdc)が小さくなるように作
用させ、前記実施例1と同様に補助電極127上でのプ
ラズマ電位を高くしたり、自己バイアス電圧(Vdc)
を少し大きくしてプラズマ中のイオンが補助電極127
に入射されるようにし、イオンの入射量を制御できるよ
うにする。補助電極127へのイオン入射の制御によっ
て、補助電極127表面でのプラズマ中の活性種との反
応を制御することも可能である。これにより、上述の可
変抵抗器(R1)を制御したときと同様の効果を得るこ
とができる。When a high frequency voltage is applied to the auxiliary electrode 127 by the substrate bias power supply 117, for example,
By suppressing the high frequency power to be applied by reducing the capacity of the capacitor C1, it is possible to suppress the inflow of ions from the plasma to the auxiliary electrode 127, and to increase the high frequency power to be applied by increasing the capacity of the capacitor C1. Thus, the flow of ions into the auxiliary electrode 127 from the plasma can be increased. Thus, the absolute value of the high-frequency self-bias voltage (Vdc) of the auxiliary electrode 127 can be controlled, so that the self-bias voltage (Vdc) is reduced, and the plasma on the auxiliary electrode 127 is actuated as in the first embodiment. Increase potential or self bias voltage (Vdc)
Is slightly increased so that the ions in the plasma
And the amount of ion incident can be controlled. By controlling the incidence of ions on the auxiliary electrode 127, it is also possible to control the reaction with the active species in the plasma on the surface of the auxiliary electrode 127. Thereby, the same effect as when the above-described variable resistor (R1) is controlled can be obtained.
【0019】上述は、可変抵抗器(R1)と可変容量コ
ンデンサ(C1)とをそれぞれ個別に制御しても良い
し、さらに最適な制御を行なうために組合わせて制御す
ることも有効である。As described above, it is effective to control the variable resistor (R1) and the variable capacitor (C1) individually, or to control the variable resistor (R1) and the variable capacitor (C1) in combination for more optimal control.
【0020】本第3の実施例によれば、補助電極127
上でのプラズマ電位を制御し、チャージングダメージの
発生を抑制するとともにスカベンジ作用によるエッチン
グの均一性を向上させることができるという効果があ
る。According to the third embodiment, the auxiliary electrode 127
By controlling the plasma potential above, there is an effect that the occurrence of charging damage can be suppressed and the uniformity of etching by the scavenging action can be improved.
【0021】上述のこれらの実施例ではエッチング装置
について述べたが、アッシング装置,プラズマCVD装
置など、基板電極へ高周波電力を供給する他のプラズマ
処理装置に同様に適用することができる。In the above embodiments, the etching apparatus has been described. However, the present invention can be similarly applied to other plasma processing apparatuses for supplying high-frequency power to the substrate electrode, such as an ashing apparatus and a plasma CVD apparatus.
【0022】[0022]
【発明の効果】本発明によれば、被処理材上のプラズマ
電位よりも基板電極外周部のプラズマ電位を高くするこ
とで、被処理材の面内の電位分布を低減することがで
き、対向する両電極のアースとしての機能が向上し、高
周波電流が処理容器内の処理室内壁よりも対向する電極
により多く流れることから、磁場を横切る方向の電流が
減少し、チャージングダメージの抑制が可能となり、半
導体デバイスの歩留まりを高め、高精度な表面処理が可
能なプラズマ処理方法および装置を提供することができ
る。According to the present invention, by making the plasma potential on the outer peripheral portion of the substrate electrode higher than the plasma potential on the material to be processed, the in-plane potential distribution of the material to be processed can be reduced. The function as a ground for both electrodes is improved, and more high-frequency current flows to the opposing electrode than the inner wall of the processing chamber in the processing chamber, reducing the current across the magnetic field and suppressing charging damage. Thus, a plasma processing method and apparatus capable of improving the yield of semiconductor devices and performing high-precision surface treatment can be provided.
【図1】本発明の第1の実施例であるプラズマ処理装置
を示す縦断面図である。FIG. 1 is a longitudinal sectional view showing a plasma processing apparatus according to a first embodiment of the present invention.
【図2】図1の装置の電位制御回路を示す図である。FIG. 2 is a diagram showing a potential control circuit of the device of FIG.
【図3】図2の電位制御回路を用いた場合のプラズマ電
位を示す図である。FIG. 3 is a diagram showing a plasma potential when the potential control circuit of FIG. 2 is used.
【図4】本発明の第2の実施例であるプラズマ処理装置
を示す縦断面図である。FIG. 4 is a longitudinal sectional view showing a plasma processing apparatus according to a second embodiment of the present invention.
【図5】本発明の第3の実施例であるプラズマ処理装置
の電位制御回路を示す図である。FIG. 5 is a diagram showing a potential control circuit of a plasma processing apparatus according to a third embodiment of the present invention.
101…真空容器、102…誘電体窓、103…アンテ
ナ電極、104…処理容器、105…処理室、106…
真空排気口、107…ガス供給装置、108…高周波電
源、109,113…フィルター、110…整合器、1
11…同軸線路、112…アンテナバイアス電源、11
4…磁場発生用コイル、115…基板電極、116…被
処理材、117…基板バイアス電源、118,119…
整合器、120…静電チャック電源、121…アンテナ
カバー、122…同軸線路、125…位相制御器、126
…電位制御回路、127…補助電極、128…制御装
置。101: vacuum container, 102: dielectric window, 103: antenna electrode, 104: processing container, 105: processing chamber, 106:
Vacuum exhaust port, 107 gas supply device, 108 high frequency power supply, 109, 113 filter, 110 matching device, 1
11 ... coaxial line, 112 ... antenna bias power supply, 11
4: coil for generating a magnetic field, 115: substrate electrode, 116: material to be processed, 117: substrate bias power supply, 118, 119
Matching device, 120: electrostatic chuck power supply, 121: antenna cover, 122: coaxial line, 125: phase controller, 126
... potential control circuit, 127 ... auxiliary electrode, 128 ... control device.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 渡辺 成一 山口県下松市大字東豊井794番地 株式会 社日立製作所笠戸事業所内 Fターム(参考) 4G075 AA24 AA30 AA62 BC04 BC06 CA25 CA26 CA47 CA65 EB01 EB41 EC21 FC11 FC15 4K030 CA04 CA12 FA02 FA04 HA16 JA16 JA17 JA18 JA19 KA15 KA19 KA20 KA30 KA41 5F004 AA01 AA06 BA14 BB07 BB11 BB14 BB23 BB32 BD01 CA03 CA06 ────────────────────────────────────────────────── ─── Continuing on the front page (72) Inventor Seiichi Watanabe 794, Higashitoyoi, Katsumatsu-shi, Yamaguchi Prefecture F-term in Kasado Works, Hitachi, Ltd. FC11 FC15 4K030 CA04 CA12 FA02 FA04 HA16 JA16 JA17 JA18 JA19 KA15 KA19 KA20 KA30 KA41 5F004 AA01 AA06 BA14 BB07 BB11 BB14 BB23 BB32 BD01 CA03 CA06
Claims (6)
排気された処理室内にプラズマを生成するとともに、前
記処理室内に設けられた基板電極にバイアス電圧を印加
し、前記プラズマの生成とは独立に前記プラズマ中のイ
オンの被処理材への入射エネルギを制御し、前記被処理
材を処理するプラズマ処理方法において、前記基板電極
外周部のプラズマ電位を前記被処理材上のプラズマ電位
よりも高くし、前記被処理材を処理することを特徴とす
るプラズマ処理方法。A plasma is generated in a processing chamber in which a processing gas is supplied and the inside of the processing chamber is depressurized and evacuated to a predetermined pressure, and a bias voltage is applied to a substrate electrode provided in the processing chamber. In the plasma processing method of controlling the incident energy of ions in the plasma to the material to be processed independently and processing the material to be processed, the plasma potential at the outer peripheral portion of the substrate electrode is made higher than the plasma potential at the material to be processed. A plasma processing method, wherein the processing target material is processed.
処理室と、前記処理室内へガスを供給するガス供給装置
と、前記処理室内に設けられ被処理材を載置可能な基板
電極と、前記処理室内に供給されたガスをプラズマ化す
る電磁波を前記処理室内に放射する第1の高周波電源
と、前記基板電極へ接続され前記被処理材に基板バイア
ス電圧を印加する第2の高周波電源とを具備するプラズ
マ処理装置において、前記基板電極に印加する高周波電
圧の正のピーク電圧に対し、その値より大きい正のピー
ク電圧が発生する補助電極を前記被処理材の外周部に設
けたことを特徴とするプラズマ処理装置。2. A processing chamber to which a vacuum evacuation device is connected and whose inside can be decompressed, a gas supply device for supplying gas into the processing chamber, a substrate electrode provided in the processing chamber and capable of mounting a material to be processed, and A first high-frequency power supply for radiating an electromagnetic wave for converting a gas supplied into the processing chamber into plasma into the processing chamber, and a second high-frequency power supply connected to the substrate electrode and applying a substrate bias voltage to the material to be processed In the plasma processing apparatus comprising: an auxiliary electrode that generates a positive peak voltage larger than the positive peak voltage of the high-frequency voltage applied to the substrate electrode on the outer peripheral portion of the workpiece; A plasma processing apparatus characterized by the above-mentioned.
て、前記第1の高周波電源を前記基板電極と電位制御回
路を介して前記補助電極に接続したことを特徴とするプ
ラズマ処理装置。3. The plasma processing apparatus according to claim 2, wherein said first high-frequency power supply is connected to said auxiliary electrode via said substrate electrode and a potential control circuit.
て、前記処理室内に前記基板電極に対向しプラズマ発生
用の電磁波を放射するアンテナ電極を設け、前記アンテ
ナ電極に第3の高周波電源を接続し、前記基板電極へ接
続された前記第1の高周波電源と前記アンテナ電極へ接
続された前記第3の高周波電源とを同一周波数とし、そ
れぞれの高周波電源の位相を制御する手段を設けたプラ
ズマ処理装置。4. The plasma processing apparatus according to claim 3, wherein an antenna electrode for radiating an electromagnetic wave for plasma generation is provided in the processing chamber so as to face the substrate electrode, and a third high frequency power supply is connected to the antenna electrode. A plasma processing apparatus, wherein the first high-frequency power supply connected to the substrate electrode and the third high-frequency power supply connected to the antenna electrode have the same frequency, and a means for controlling the phase of each high-frequency power supply is provided. .
排気された処理室内にプラズマを生成するとともに、前
記処理室内に設けられた基板電極にバイアス電圧を印加
し、前記プラズマの生成とは独立に前記プラズマ中のイ
オンの被処理材への入射エネルギを制御し、前記被処理
材を処理するプラズマ処理方法において、前記基板電極
外周部のプラズマ電位を前記被処理材上のプラズマ電位
よりも高くするとともに、前記基板電極外周部でスカベ
ンジ作用を生じさせ前記被処理材を処理することを特徴
とするプラズマ処理方法。5. A plasma is generated in a processing chamber in which a processing gas is supplied and the inside of the processing chamber is evacuated to a predetermined pressure, and a bias voltage is applied to a substrate electrode provided in the processing chamber. In the plasma processing method of controlling the incident energy of ions in the plasma to the material to be processed independently and processing the material to be processed, the plasma potential at the outer peripheral portion of the substrate electrode is made higher than the plasma potential at the material to be processed. A plasma processing method comprising: increasing the height of the substrate; and causing a scavenging effect at an outer peripheral portion of the substrate electrode to process the material to be processed.
処理室と、前記処理室内へガスを供給するガス供給装置
と、前記処理室内に設けられ被処理材を載置可能な基板
電極と、前記処理室内に供給されたガスをプラズマ化す
る電磁波を前記処理室内に放射する第1の高周波電源
と、前記基板電極へ接続され前記被処理材に基板バイア
ス電圧を印加する第2の高周波電源とを具備するプラズ
マ処理装置において、前記基板電極に印加する高周波電
圧の正のピーク電圧に対し、その値より大きい正のピー
ク電圧が発生されるとともに、プラズマ中のイオンが入
射されプラズマ中の活性種と反応する材料でなる補助電
極を前記被処理材の外周部に設けたことを特徴とするプ
ラズマ処理装置。6. A processing chamber to which a vacuum evacuation device is connected and whose inside can be depressurized, a gas supply device for supplying a gas into the processing chamber, a substrate electrode provided in the processing chamber and capable of mounting a material to be processed. A first high-frequency power supply for radiating an electromagnetic wave for converting a gas supplied into the processing chamber into plasma into the processing chamber, and a second high-frequency power supply connected to the substrate electrode and applying a substrate bias voltage to the material to be processed And a positive peak voltage higher than the positive peak voltage of the high-frequency voltage applied to the substrate electrode is generated, and ions in the plasma are injected to activate the plasma in the plasma. A plasma processing apparatus, wherein an auxiliary electrode made of a material that reacts with a seed is provided on an outer peripheral portion of the material to be processed.
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| JP2001004371A JP3599670B2 (en) | 2001-01-12 | 2001-01-12 | Plasma processing method and apparatus |
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|---|---|---|---|
| JP2001004371A JP3599670B2 (en) | 2001-01-12 | 2001-01-12 | Plasma processing method and apparatus |
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| JP3599670B2 JP3599670B2 (en) | 2004-12-08 |
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Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2004111432A (en) * | 2002-09-13 | 2004-04-08 | Hitachi High-Technologies Corp | Plasma processing apparatus and plasma processing method |
| JP2010531538A (en) * | 2007-03-05 | 2010-09-24 | ラム リサーチ コーポレーション | Edge electrode with variable power |
| KR101343967B1 (en) * | 2012-07-06 | 2013-12-20 | 가부시키가이샤 히다치 하이테크놀로지즈 | Plasma processing apparatus and method |
| JP2017503314A (en) * | 2013-12-17 | 2017-01-26 | 東京エレクトロン株式会社 | System and method for controlling plasma density |
| JP2019537272A (en) * | 2016-12-02 | 2019-12-19 | エーエスエムエル ネザーランズ ビー.ブイ. | How to change etching parameters |
| WO2025069651A1 (en) * | 2023-09-29 | 2025-04-03 | 東京エレクトロン株式会社 | Plasma processing device |
-
2001
- 2001-01-12 JP JP2001004371A patent/JP3599670B2/en not_active Expired - Fee Related
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2004111432A (en) * | 2002-09-13 | 2004-04-08 | Hitachi High-Technologies Corp | Plasma processing apparatus and plasma processing method |
| JP2010531538A (en) * | 2007-03-05 | 2010-09-24 | ラム リサーチ コーポレーション | Edge electrode with variable power |
| KR101343967B1 (en) * | 2012-07-06 | 2013-12-20 | 가부시키가이샤 히다치 하이테크놀로지즈 | Plasma processing apparatus and method |
| JP2017503314A (en) * | 2013-12-17 | 2017-01-26 | 東京エレクトロン株式会社 | System and method for controlling plasma density |
| JP2019537272A (en) * | 2016-12-02 | 2019-12-19 | エーエスエムエル ネザーランズ ビー.ブイ. | How to change etching parameters |
| US11300887B2 (en) | 2016-12-02 | 2022-04-12 | Asml Netherlands B.V. | Method to change an etch parameter |
| JP7057358B2 (en) | 2016-12-02 | 2022-04-19 | エーエスエムエル ネザーランズ ビー.ブイ. | How to change etching parameters and computer program |
| WO2025069651A1 (en) * | 2023-09-29 | 2025-04-03 | 東京エレクトロン株式会社 | Plasma processing device |
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| Publication number | Publication date |
|---|---|
| JP3599670B2 (en) | 2004-12-08 |
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