JPH07263531A - Plasma processing apparatus having a mechanism for separating a substrate to be electrostatically adsorbed and a method for separating a substrate to be electrostatically adsorbed to be processed - Google Patents
Plasma processing apparatus having a mechanism for separating a substrate to be electrostatically adsorbed and a method for separating a substrate to be electrostatically adsorbed to be processedInfo
- Publication number
- JPH07263531A JPH07263531A JP424095A JP424095A JPH07263531A JP H07263531 A JPH07263531 A JP H07263531A JP 424095 A JP424095 A JP 424095A JP 424095 A JP424095 A JP 424095A JP H07263531 A JPH07263531 A JP H07263531A
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- Prior art keywords
- substrate
- processed
- gas
- separating
- electrostatic attraction
- Prior art date
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Abstract
(57)【要約】
【目的】 静電吸着電極から被処理基板を迅速、確実且
つ安全に離脱出来る機構を備えたプラズマ処理装置およ
び被処理基板の離脱方法を提供することを目的としてい
る。
【構成】 静電吸着クランプ機構を備えたプラズマ処理
装置において、真空槽10に静電吸着電極面から突出可
能なリフトピン9と、空気、希ガス、無機ガス、もしく
は窒素、酸素、水素、イオウ、塩素またはフッ素原子の
うち少なくとも1種を含むガスの1つ又は複数の混合ガ
スの導入機構1を備え、混合ガスの圧力を所定の圧力に
保持するための圧力制御系7、7a、7bを有する装置
である。被処理基板5を離脱する際、リフトピン9で離
脱力を与えると共に、前記混合ガスの圧力を所定の圧力
(0.1〜500Pa)に維持する。
(57) [Abstract] [Purpose] An object of the present invention is to provide a plasma processing apparatus and a method for separating a substrate to be processed, which is provided with a mechanism capable of quickly, reliably and safely separating the substrate to be processed from the electrostatic adsorption electrode. In a plasma processing apparatus provided with an electrostatic adsorption clamp mechanism, a lift pin 9 capable of projecting from an electrostatic adsorption electrode surface into a vacuum chamber 10 and air, a rare gas, an inorganic gas, or nitrogen, oxygen, hydrogen, sulfur, It has a mechanism 1 for introducing one or more mixed gases of gases containing at least one of chlorine or fluorine atoms, and has pressure control systems 7, 7a, 7b for maintaining the pressure of the mixed gases at a predetermined pressure. It is a device. When the substrate 5 to be processed is detached, the lift pin 9 applies a detaching force, and the pressure of the mixed gas is maintained at a predetermined pressure (0.1 to 500 Pa).
Description
【0001】[0001]
【産業上の利用分野】本発明は、半導体製造装置等に応
用されるプラズマ処理装置に関する。より詳細には静電
吸着電極から被処理基板を迅速、確実且つ安全に離脱出
来る機構を備えたプラズマ処理装置および被処理基板の
離脱方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a plasma processing apparatus applied to a semiconductor manufacturing apparatus or the like. More specifically, the present invention relates to a plasma processing apparatus having a mechanism capable of quickly, reliably and safely detaching a substrate to be processed from an electrostatic attraction electrode and a method of detaching the substrate to be processed.
【0002】[0002]
【従来の技術】減圧下で半導体ウエハ等の被処理基板の
表面加工処理を行なうプラズマ処理装置においては、プ
ラズマから被処理基板が受ける熱を効率良く奪い、被処
理基板が温度上昇により不可逆的なダメージを受けるこ
とを防止するため、被処理基板を支持する電極の温度の
上昇を防止する温調機構と、被処理基板と電極との熱伝
導の効率を上げる手段を備える必要がある。被処理基板
と電極との熱伝導の効率を上げる手段としては、被処理
基板の上から機械的に力を電極に向けて加えて固定す
る、所謂メカニカルクランプ機構や、電極上に誘電体を
介して被処理基板を置き、前記電極と被処理基板との間
に直流電圧を印加したり、プラズマにより被処理基板に
誘起される自己バイアス電圧により、静電吸着による固
定を行なう静電吸着クランプ機構により被処理基板と電
極との間隔を狭め、接触面積を増加させる方法や、これ
らの機構に加えて、被処理基板と電極との間隙をHe等
のガスで満たし、対流を発生させる方法が知られてい
る。2. Description of the Related Art In a plasma processing apparatus for processing the surface of a substrate to be processed such as a semiconductor wafer under reduced pressure, the heat received by the substrate to be processed is efficiently removed from the plasma, and the temperature of the substrate to be processed is irreversible. In order to prevent damage, it is necessary to provide a temperature control mechanism for preventing the temperature of the electrode supporting the substrate to be processed from rising and a means for increasing the efficiency of heat conduction between the substrate to be processed and the electrode. As means for increasing the efficiency of heat conduction between the substrate to be processed and the electrodes, a mechanical clamping mechanism for mechanically applying force to the electrode from above the substrate to be fixed, which is called a mechanical clamp mechanism, or a dielectric on the electrode is used. A substrate to be processed is placed, and a DC voltage is applied between the electrode and the substrate to be processed, or a self-bias voltage induced on the substrate to be processed by plasma is used to fix the substrate by electrostatic attraction. There is known a method of narrowing the distance between the substrate to be processed and the electrode to increase the contact area, and a method of generating convection by filling the gap between the substrate to be processed and the electrode with a gas such as He in addition to these mechanisms. Has been.
【0003】しかしながら、最近は被処理基板が大型化
する傾向にある上、基板の有効利用面積の拡大の要請が
高まっているため、メカニカルクランプではより小さく
かつ少数のクランプ用爪を基板の縁部に近いところで使
って基板を電極に押し付けなくてはならず、基板のひず
みが発生し、また被処理基板と電極との熱伝導の向上に
ガスを併用する場合にはガス圧を所望の値に保持出来な
いなどの不都合があった。また、クランプのための爪と
被処理基板との機械的接触や、クランプのための爪に付
着した反応生成物の剥離などによりパーティクルが発生
しやすくなるという問題がある。However, recently, the size of the substrate to be processed tends to be large, and the demand for expansion of the effective use area of the substrate is increasing. Therefore, in the mechanical clamp, a smaller and smaller number of clamping claws are provided on the edge of the substrate. The substrate must be pressed against the electrode by using it close to the plate, the substrate will be distorted, and if the gas is used together to improve the heat conduction between the substrate to be processed and the electrode, set the gas pressure to the desired value. There was an inconvenience such as being unable to hold it. Further, there is a problem that particles are likely to be generated due to mechanical contact between the claw for clamping and the substrate to be processed, peeling of the reaction product attached to the claw for clamping, and the like.
【0004】これに対し静電吸着による被処理基板の固
定方法はプラズマを乱すことなく被処理基板の全面に亘
って均等な力で固定することが出来、本質的に大型の被
処理基板に適した固定方法である。On the other hand, the method of fixing the substrate to be processed by electrostatic attraction can fix the substrate to be processed with uniform force over the entire surface without disturbing the plasma, and is essentially suitable for a large substrate to be processed. It is a fixed method.
【0005】しかしながら、静電吸着クランプ機構を用
いる場合、被処理基板と静電吸着電極との間に介在する
誘電体内の残留電荷により生ずる電位差のために、プラ
ズマ処理終了後も吸着力が減少せず、被処理基板を迅
速、確実且つ安全に離脱することが困難である。However, when the electrostatic adsorption clamp mechanism is used, the adsorption force is reduced even after the plasma processing is completed due to the potential difference caused by the residual charges in the dielectric substance interposed between the substrate to be processed and the electrostatic adsorption electrode. Therefore, it is difficult to remove the substrate to be processed quickly, reliably and safely.
【0006】従来、静電吸着された被処理基板を離脱す
る方法としては、大別して次の2種がある。Conventionally, there are roughly the following two types of methods for removing the electrostatically attracted substrate to be processed.
【0007】(1) 機械的手段による離脱機構 (1−1) 静電吸着電極表面からピンもしくはピスト
ン等の機械的離脱力付与手段を突出させる方法。 (1−2) 高圧力のガスを静電吸着電極内部に設けた
導入管より、被処理基板と静電吸着電極との間隙に導入
し、ガス圧の膨張力をもって離脱力を付与する方法。 (2) 電気的手段による離脱機構 (2−1) 静電吸着電極と被処理基板に印加する電圧
の極性を反転することにより、両者に介在する絶縁物の
残留電荷を消去させて吸着力の消滅を図る方法。 (2−2) 静電吸着電極と被処理基板の電位を接地電
位にし、吸着力の消滅を図る方法。 (2−3) 被処理基板が半導体ウエハの場合には、プ
ラズマが存在する状態で直流電圧をゼロにしてプラズマ
を介して残留電荷を消失させる方法。(1) Detachment mechanism by mechanical means (1-1) A method of causing a mechanical detachment force applying means such as a pin or a piston to protrude from the surface of the electrostatic attraction electrode. (1-2) A method in which a high-pressure gas is introduced into the gap between the substrate to be processed and the electrostatic adsorption electrode from an introduction tube provided inside the electrostatic adsorption electrode, and the desorption force is imparted by the expansive force of the gas pressure. (2) Detachment mechanism by electric means (2-1) By reversing the polarity of the voltage applied to the electrostatic attraction electrode and the substrate to be processed, the residual charge of the insulator interposed between the two is erased and the attraction force is increased. How to eliminate it. (2-2) A method in which the potential of the electrostatic attraction electrode and the substrate to be processed are set to the ground potential to eliminate the attraction force. (2-3) In the case where the substrate to be processed is a semiconductor wafer, a method in which the DC voltage is set to zero in the presence of plasma and the residual charges are eliminated through the plasma.
【0008】[0008]
【発明が解決しようとする課題】しかし、上記の各種従
来技術には、いずれも原理的もしくは実用上次のような
問題があった。However, each of the above-mentioned various conventional techniques has the following problems in principle or in practical use.
【0009】(1) 機械的手段による強制的離脱によ
る問題点 (1−1) 静電吸着電極表面から突出可能なピンもし
くはピストン等の機械的離脱力付与手段を突出させる方
法は、残留電荷による吸着力が被処理基板全面に均等に
作用している状態で被処理基板の一部に離脱する力を無
理に加える。この為、その力が加えられた部分で、被処
理基板の変形や破壊を招く可能性が大きい。 (1−2) また、機械的離脱機構と被処理基板とが接
触摩擦されることによるパーティクルの発生という問題
もある。 (1−3) ガス圧の膨張力により被処理基板を離脱さ
せる場合、被処理基板が、例えばシリコンウエハのよう
に軽い被処理基板においては、離脱の瞬間、ウエハが吹
き上げられ、著しくはウエハの破損に至る難点があっ
た。(1) Problems due to forced disengagement by mechanical means (1-1) The method of causing a mechanical disengagement force imparting means such as a pin or a piston capable of protruding from the surface of the electrostatic adsorption electrode is caused by residual charge. A force for detaching a part of the substrate to be processed is forcibly applied in a state where the suction force uniformly acts on the entire surface of the substrate to be processed. Therefore, there is a high possibility that the portion to which the force is applied may deform or break the substrate to be processed. (1-2) Further, there is a problem that particles are generated due to contact friction between the mechanical separation mechanism and the substrate to be processed. (1-3) When the substrate to be processed is separated by the expansion force of gas pressure, if the substrate to be processed is a light substrate such as a silicon wafer, the wafer is blown up at the moment of separation, and significantly There was a point of failure.
【0010】(2) 電気的手段による残留電荷消去の
問題点 (2−1) 印加電圧の極性反転により絶縁体中の残留
電荷を消去させようとする場合、ただ1回の極性反転に
よって残留電荷を過不足なしの完全消去状態とすること
は実際上困難である。これを克服するため、印加電圧の
極性を繰返し反転させつつ、徐々にその値を小さくして
ゆき、最終的にゼロにするというプロセスが不可避であ
った。このためこの極性反転法のみによるならば、離脱
を行うために必ず数十秒以上の長時間を要する。 (2−2) 静電吸着電極と被処理基板をともに接地す
る方法は、被処理基板の裏面に誘電体の薄膜、例えば、
SiO2 膜が存在する場合、その誘電体膜の残留電荷を
完全になくすまでの時定数が非常に大きく、実用的でな
い。 (2−3) プラズマが存在する状態で直流電圧をゼロ
にしてプラズマを介して残留電荷を消失させる方法は、
吸着力の減少により被処理基板と静電吸着電極との熱伝
導が悪化し、被処理基板の温度上昇を招くおそれがあ
る。また、直流電圧をゼロにしてプラズマの存在する時
間の設定が不適切であると、残留電荷が多く残っていた
り、被処理基板に生ずる自己バイアスにより再度帯電し
たりして、吸着力を充分に下げることができない。(2) Problems of Eliminating Residual Charge by Electrical Means (2-1) When erasing the residual charge in the insulator by reversing the polarity of the applied voltage, the residual charge is eliminated only once. It is practically difficult to set the state to the completely erased state without excess or deficiency. In order to overcome this, it was inevitable that the polarity of the applied voltage was repeatedly inverted, the value was gradually decreased, and finally the value was made zero. Therefore, if only the polarity reversal method is used, it takes a long time of several tens of seconds or more to perform separation. (2-2) A method of grounding both the electrostatic attraction electrode and the substrate to be processed is as follows.
When the SiO 2 film is present, the time constant until completely eliminating the residual charges of the dielectric film is very large, which is not practical. (2-3) A method in which the DC voltage is set to zero in the presence of plasma and the residual charge is eliminated through the plasma is as follows.
Due to the decrease in the attraction force, the heat conduction between the substrate to be processed and the electrostatic attraction electrode may be deteriorated, and the temperature of the substrate to be processed may rise. In addition, if the DC voltage is set to zero and the time during which the plasma is present is set improperly, a large amount of residual charge remains or the substrate is recharged due to self-bias generated on the substrate to be processed, and the adsorption force is sufficiently increased. I can't lower it.
【0011】以上の如くの問題点に鑑みてなされた本発
明は、静電吸着電極から被処理基板を迅速、確実且つ安
全に離脱出来る機構を備えたプラズマ処理装置および被
処理基板の離脱方法を提供することを目的としている。The present invention, which has been made in view of the above problems, provides a plasma processing apparatus and a method for removing a substrate to be processed, which is provided with a mechanism capable of quickly, reliably and safely removing the substrate to be processed from the electrostatic attraction electrode. It is intended to be provided.
【0012】[0012]
【課題を解決するための手段】本発明は、前記問題点を
解決するために、電極上に誘電体を介して被処理基板を
置き、前記電極と被処理基板との間の直流電位差による
静電吸着によって被処理基板の固定を行なう静電吸着ク
ランプ機構を備え、減圧下で被処理基板の加工処理を行
なうプラズマ処理装置において、被処理基板の離脱動作
が行なわれるチャンバーに、静電吸着電極面から突出可
能なピンもしくはピストン等の機械的離脱力付与手段
と、空気、希ガス、無機ガスもしくは窒素、酸素、水
素、イオウ、塩素またはフッ素原子のうち少なくとも1
種を含む混合ガスを被処理基板周辺に供給する為のガス
導入機構とを備えると共に、被処理基板の離脱動作が行
なわれるチャンバー内の圧力を所定の圧力に保持するた
めの圧力制御系を備えたことを特徴とする。In order to solve the above-mentioned problems, the present invention places a substrate to be processed on an electrode via a dielectric, and a static electricity caused by a DC potential difference between the electrode and the substrate to be processed. In a plasma processing apparatus equipped with an electrostatic adsorption clamp mechanism for fixing a substrate to be processed by electroadsorption and performing processing of the substrate to be processed under reduced pressure, an electrostatic adsorption electrode is placed in a chamber where the substrate to be processed is detached. A mechanical releasing force applying means such as a pin or a piston capable of projecting from the surface, and at least one of air, a rare gas, an inorganic gas or nitrogen, oxygen, hydrogen, sulfur, chlorine or a fluorine atom.
A gas introduction mechanism for supplying a mixed gas containing seeds to the periphery of the substrate to be processed, and a pressure control system for maintaining the pressure in the chamber where the substrate to be processed is released at a predetermined pressure. It is characterized by that.
【0013】機械的離脱力付与手段、ガス導入機構およ
び圧力制御系に対するシーケンサを更に備えるのが、動
作の自動化の点で望ましい。It is desirable from the standpoint of automation of operation to further include a sequencer for the mechanical releasing force applying means, the gas introduction mechanism and the pressure control system.
【0014】機械的離脱力付与手段は、静電吸着電極の
吸着面内の、被処理基板の縁部以外と対向する位置に設
けるのが好ましい。この機械的離脱力付与手段は、たと
えば、前記吸着面内の、円周に沿って、等間隔で、突没
自在に設けた複数のピンで構成する。また、別な例とし
て、吸着面内に、吸着面と面一で、突没自在に設けた円
形台で構成する。It is preferable that the mechanical separating force applying means is provided at a position in the attraction surface of the electrostatic attraction electrode, which is opposed to a portion other than the edge portion of the substrate to be processed. The mechanical separating force applying means is composed of, for example, a plurality of pins provided at the suction surface along the circumference at regular intervals so as to be capable of projecting and retracting. Further, as another example, it is configured by a circular base provided in the suction surface so as to be flush with the suction surface so as to be retractable.
【0015】さらに、好ましくは、機械的離脱力付与手
段に、ピンまたは円形台の吸着面から突出する高さを調
節する駆動機構を設ける。Further, preferably, the mechanical releasing force applying means is provided with a drive mechanism for adjusting the height of the pin or the circular base protruding from the suction surface.
【0016】また、本発明の静電吸着された被処理基板
の離脱方法は、前記の如くのプラズマ処理装置におい
て、静電吸着電極に静電吸着により固定された被処理基
板を離脱する方法であって、前記被処理基板に静電吸着
電極の吸着面から突出可能なピンもしくはピストン等の
機械的離脱力付与手段を用いて離脱力を与えると共に、
被処理基板の近傍において空気、希ガス、無機ガスもし
くは窒素、酸素、水素、イオウ、塩素またはフッ素原子
のうち少なくとも1種を含む混合ガスの所定圧力雰囲気
を維持することを特徴としている。Further, the method of releasing the electrostatically adsorbed substrate to be processed is a method of releasing the substrate to be processed which is fixed to the electrostatic adsorption electrode by electrostatic adsorption in the plasma processing apparatus as described above. There is a detaching force applied to the substrate to be processed by using a mechanical detaching force imparting means such as a pin or a piston capable of protruding from the attraction surface of the electrostatic attraction electrode,
It is characterized in that a predetermined pressure atmosphere of air, a rare gas, an inorganic gas or a mixed gas containing at least one of nitrogen, oxygen, hydrogen, sulfur, chlorine or fluorine atoms is maintained in the vicinity of the substrate to be processed.
【0017】また、静電吸着により電極に固定された被
処理基板と静電吸着電極の吸着面との間に微間隙を形成
することで、その微間隙の形成により被処理基板と静電
吸着電極との間の電位差を増大させ、被処理基板周辺の
雰囲気中に存在するガス(以下「雰囲気ガス」と呼ぶ)
を放電用ガスとして、被処理基板近傍で放電を発生させ
る。その放電により帯電したガス粒子が、帯電した被処
理基板を除電する。そして、この除電後に被処理基板を
静電吸着電極から引き離すことを特徴としている。Further, by forming a minute gap between the substrate to be processed fixed to the electrode by electrostatic attraction and the attraction surface of the electrostatic attraction electrode, the substrate to be treated and the electrostatic attraction by the formation of the minute gap. Gas that increases the potential difference between the electrodes and exists in the atmosphere around the substrate to be processed (hereinafter referred to as "atmosphere gas")
Is used as a discharge gas to generate a discharge near the substrate to be processed. The gas particles charged by the discharge neutralize the charged substrate to be processed. Then, after the static elimination, the substrate to be processed is separated from the electrostatic attraction electrode.
【0018】被処理基板の近傍で放電を発生させるため
に、被処理基板と静電吸着電極間の電位差が放電開始電
圧以上となるように、その微間隙を設定し、さらにパッ
センの法則に従って、その雰囲気ガスの圧力を設定す
る。微間隙を設定した後圧力を設定する場合と、圧力を
設定した後、微間隙を設定する場合がある。In order to generate an electric discharge in the vicinity of the substrate to be processed, the fine gap is set so that the potential difference between the substrate to be processed and the electrostatic adsorption electrode becomes equal to or higher than the discharge start voltage, and further according to Passen's law, The pressure of the atmosphere gas is set. There are cases where the pressure is set after setting the fine gap, and cases where the fine gap is set after setting the pressure.
【0019】前記微間隙の間隔は、約0.1mm以上か
ら約1mm以下に設定することが好ましい。The interval of the fine gap is preferably set to about 0.1 mm or more and about 1 mm or less.
【0020】この微間隙の間隔の範囲内で、雰囲気ガス
の圧力は、0.1Paから500Paに設定することが
好ましい。It is preferable that the pressure of the atmospheric gas is set to 0.1 Pa to 500 Pa within the range of the fine gap.
【0021】被処理基板と静電吸着電極間に生じる電位
差は、その微間隙の間隔に比例する。被処理基板近傍に
発生する放電は、DC放電である。The potential difference between the substrate to be processed and the electrostatic attraction electrode is proportional to the interval of the minute gap. The discharge generated in the vicinity of the substrate to be processed is DC discharge.
【0022】放電後、被処理基板と静電吸着電極との電
位差が放電維持電位以下になったときに、被処理基板を
静電吸着電極から引き離す。たとえば、8インチの被処
理基板でその表面電位が220V以下となったときに被
処理基板を静電吸着電極から引き離す。After the discharge, when the potential difference between the substrate to be treated and the electrostatic attraction electrode becomes equal to or lower than the discharge sustaining potential, the substrate to be treated is separated from the electrostatic attraction electrode. For example, when the surface potential of an 8-inch substrate to be processed becomes 220 V or less, the substrate to be processed is separated from the electrostatic attraction electrode.
【0023】雰囲気ガスとして好ましくは、流量200
sccm、圧力20Paで窒素ガスを導入する。The atmosphere gas preferably has a flow rate of 200.
Nitrogen gas is introduced at a sccm pressure of 20 Pa.
【0024】または、雰囲気ガスは、被処理基板を処理
するガスとする。たとえば、被処理基板を処理するガス
をCF4 +O2 、または、CF4 +CHF3 とする。Alternatively, the atmospheric gas is a gas for processing the substrate to be processed. For example, the gas for processing the substrate to be processed is CF 4 + O 2 or CF 4 + CHF 3 .
【0025】被処理基板と静電吸着電極との間に微間隙
を形成するために、静電吸着電極面からピンが突出す
る。In order to form a fine gap between the substrate to be processed and the electrostatic attraction electrode, the pin projects from the surface of the electrostatic attraction electrode.
【0026】このピンの高さは、被処理基板が破損しな
い程度の高さに調整する。好ましくは、ピンの高さを、
約0.1mm以上から約1mm以下に設定する。The height of this pin is adjusted to such a level that the substrate to be processed is not damaged. Preferably, the pin height is
It is set to about 0.1 mm or more and about 1 mm or less.
【0027】[0027]
【作用】本発明にとって、被処理基板の近傍でDC放電
を発生させることがもっとも重要な役割をはたす。この
DC放電によって帯電した気体分子が、帯電した被処理
基板を除電する。In the present invention, the generation of DC discharge in the vicinity of the substrate to be processed plays the most important role. The gas molecules charged by this DC discharge neutralize the charged substrate to be processed.
【0028】このDC放電を発生させる条件は、アー
スに対する被処理基板の電位差Φs、被処理基板近傍
のアースされた部品、たとえば対向電極または真空容器
の壁面と被処理基板との距離Dおよび被処理基板周辺
に存在するガスの圧力Pとによって定められる。より詳
細には、アースに対する被処理基板の電位差Φs が、パ
ッセンの法則(またはパッセンの曲線(Paschen
´s law))に従って、圧力と距離との積(P*
D)で定められる放電開始電圧(Vs=f(P*D))
と同じかまたはそれ以上のとき(Φs ≧Vs)に、被処
理基板と基板近傍のアースされた部品との間にDC放電
が発生する。The conditions for generating this DC discharge are the potential difference Φ s of the substrate to be processed with respect to the ground, the distance D between the grounded component near the substrate to be processed, such as the counter electrode or the wall of the vacuum container and the substrate to be processed, and the object to be processed. It is determined by the pressure P of the gas existing around the processing substrate. More specifically, the potential difference Φ s of the substrate to be processed with respect to the earth is the Passen's law (or the Passen curve (Paschen's curve)).
('S law)), the product of pressure and distance (P *
Discharge start voltage (Vs = f (P * D)) determined by D)
When Φ s ≧ Vs or more (Φ s ≧ Vs), a DC discharge occurs between the substrate to be processed and a grounded component near the substrate.
【0029】さらに、本発明にとって、帯電した被処理
基板と静電吸着用電極との間隔(微間隙)によって、被
処理基板と静電吸着電極間の電位差を増加させること
も、DC放電を発生させるうえで重要な役割をはたす。
このような電位差が増加する現象は、理論的に、以下の
ように説明できる。アースに対する被処理基板の電位差
Φs と静電吸着用電極の電位差Φd 間の電位差V=Φs
−Φdは被処理基板の残留電荷の電気量Qと、 V=Q/C (a) の関係がある。ここで、Cは静電容量を示す。一方、静
電容量Cは、 C=εS/d (b) で示される。ここで、εは被処理基板と静電吸着電極間
の誘電率、Sは被処理基板の面積、dは被処理基板と静
電吸着電極との間隔(微間隙)を示す。(b)式を
(a)式に代入すると、 V=Qd/εS=kd (c)(kは定数) となる。ここで、被処理基板の残留電荷の電気量は、被
処理基板が接地でもされなければ減ることはないので、
Qは一定とみなすことができる。εは定数、Sも一定と
みなすことができるので、結局、被処理基板と静電吸着
電極間の電位差Vは、被処理基板と静電吸着電極との間
隔d(図3参照)に比例するといえる。したがって、被
処理基板と静電吸着電極との間隔dがひろがると、被処
理基板と静電吸着電極間の電位差Vが大きくなる。Further, according to the present invention, the potential difference between the substrate to be processed and the electrostatic attraction electrode is increased by the distance (fine gap) between the charged substrate to be treated and the electrostatic attraction electrode, and DC discharge is generated. Play an important role in making it happen.
The phenomenon that the potential difference increases can be theoretically explained as follows. The potential difference V = Φ s between the potential difference Φ s of the substrate to be ground and the potential difference Φ d of the electrostatic attraction electrode.
-Φ d has a relationship of V = Q / C (a) with the electric quantity Q of the residual charge of the substrate to be processed. Here, C represents capacitance. On the other hand, the capacitance C is represented by C = εS / d (b). Here, ε is the dielectric constant between the substrate to be processed and the electrostatic attraction electrode, S is the area of the substrate to be treated, and d is the interval (fine gap) between the substrate to be processed and the electrostatic attraction electrode. By substituting the equation (b) into the equation (a), it becomes V = Qd / εS = kd (c) (k is a constant). Here, the electric quantity of the residual charge of the substrate to be processed does not decrease unless the substrate to be processed is grounded.
Q can be regarded as constant. Since ε can be regarded as a constant and S can be regarded as constant, after all, the potential difference V between the substrate to be processed and the electrostatic attraction electrode is proportional to the distance d (see FIG. 3) between the substrate to be processed and the electrostatic attraction electrode. I can say. Therefore, when the distance d between the substrate to be processed and the electrostatic attraction electrode is increased, the potential difference V between the substrate to be processed and the electrostatic attraction electrode becomes large.
【0030】さらに、被処理基板と静電吸着電極との間
隔dがひろがることは、アースに対する被処理基板の電
位差Φs が大きくなることを意味する。静電吸着電極の
残留電荷Qから発生する電場E(=V/d=Q/εS=
一定)は、被処理基板と静電吸着電極間の間隔dがひろ
がると、大きくなるといえる。 E=V/(D−d) (d) (Dは真空容器の壁面と静電吸着電極の吸着面の間の距
離と考える。)であり、前記(c)式を代入すると E=kd/(D−d) (e) となるからである。また、アースに対する被処理基板の
電位差Φs は、電位差Vが大きくなれば、大きくなると
も言える。Further, the widening of the distance d between the substrate to be processed and the electrostatic attraction electrode means that the potential difference Φ s of the substrate to be processed with respect to the ground becomes large. Electric field E (= V / d = Q / εS = generated from residual charge Q of the electrostatic adsorption electrode)
It can be said that the constant value increases as the distance d between the substrate to be processed and the electrostatic attraction electrode increases. E = V / (D−d) (d) (D is considered to be the distance between the wall surface of the vacuum container and the adsorption surface of the electrostatic adsorption electrode.) Substituting the equation (c), E = kd / This is because (D-d) (e). It can also be said that the potential difference Φ s of the substrate to be processed with respect to the ground increases as the potential difference V increases.
【0031】以上の観点から、たとえばピンを静電吸着
電極の吸着面から突き上げて被処理基板を持ち上げる場
合、被処理基板が持ち上がっていく過程で、アースに対
する被処理基板の電位差Φs が、被処理基板と被処理基
板近傍のどこかのアースされた部品との距離D(たとえ
ば、被処理基板と対向電極との距離)と、被処理基板周
辺の雰囲気ガスの圧力Pで定まる放電開始電圧Vsに達
する。そのときに被処理基板と被処理基板近傍の部品と
の間にDC放電が発生するといえる。被処理基板近傍の
どこで放電が発生するかは、被処理基板が持ち上がって
いく過程(電位差V、すなわち基板の電位Φs が増加す
る過程)で、被処理基板と被処理基板近傍のアースされ
た部品の間の空間のうちで、最初にパッセンの法則に従
った雰囲気にある空間で発生する。From the above viewpoints, for example, when the pins are pushed up from the attraction surface of the electrostatic attraction electrode to lift the substrate to be processed, the potential difference Φ s of the substrate to be processed with respect to the ground is increased during the process of lifting the substrate to be processed. The discharge start voltage Vs determined by the distance D between the processing substrate and some grounded component near the processing substrate (for example, the distance between the processing substrate and the counter electrode) and the pressure P of the atmospheric gas around the processing substrate. Reach At that time, it can be said that DC discharge occurs between the substrate to be processed and the components near the substrate to be processed. Where the discharge occurs near the substrate to be processed is that the substrate to be processed is grounded in the vicinity of the substrate to be processed during the process of raising the substrate to be processed (potential difference V, that is, the process of increasing the potential Φ s of the substrate). Of the spaces between the parts, it first occurs in a space that has an atmosphere according to Passen's law.
【0032】しかし、被処理基板と静電吸着用電極との
間隔を無制限にひろげることはできない。被処理基板と
静電吸着電極との間隔をひろげようとすると、被処理基
板が変形または破壊するからである。間隔をひろげるた
めには、離脱するための力をより大きく加える必要があ
る。残留電荷による吸着力が被処理基板全面に均等に作
用している状態で、大きな力が部分的に加えられると、
その力が加えられた部分で容易に被処理基板がしなるか
または折れる。したがって、被処理基板が変形または破
壊しない程度に被処理基板と静電吸着電極との間隔を設
定しなければならない。被処理基板と静電吸着電極とに
微間隙を形成する程度で、被処理基板と静電吸着電極を
離すのがもっともよい。この基板離脱方法を実施する離
脱機構には、被処理基板を破損しないで被処理基板と静
電吸着電極との間に微間隙を形成する程度にピンの突き
出しの高さを調整する駆動機構を備えるのが望ましい。
さらに、ピンが被処理基板の縁部以外の部分で持ち上げ
るように配置されていなければならない。発明者らは、
被処理基板の縁部をもちげようとすると被処理基板の縁
部が欠けたり、被処理基板が傾いて上がることが基板離
脱の実験で知りえたからである。However, the distance between the substrate to be processed and the electrode for electrostatic attraction cannot be expanded indefinitely. This is because if the distance between the substrate to be processed and the electrostatic attraction electrode is increased, the substrate to be processed will be deformed or destroyed. In order to widen the space, it is necessary to apply a larger force for separation. When a large force is partially applied while the attracting force due to the residual charge acts evenly on the entire surface of the substrate to be processed,
The substrate to be processed is easily bent or broken at the portion to which the force is applied. Therefore, the distance between the substrate to be processed and the electrostatic attraction electrode must be set so that the substrate to be processed is not deformed or destroyed. It is best to separate the substrate to be processed and the electrostatic adsorption electrode to the extent that a minute gap is formed between the substrate to be processed and the electrostatic adsorption electrode. The detachment mechanism that implements this substrate detachment method includes a drive mechanism that adjusts the protrusion height of the pins to the extent that a fine gap is formed between the substrate to be processed and the electrostatic attraction electrode without damaging the substrate to be processed. It is desirable to be prepared.
Further, the pins must be arranged so as to be lifted at a portion other than the edge portion of the substrate to be processed. The inventors
This is because it was found from the substrate detachment experiment that the edge of the substrate to be processed was chipped or the substrate to be processed tilted up when the edge of the substrate to be processed was lifted.
【0033】被処理基板と静電吸着電極との間が、微間
隙を形成する程度の距離しか設定できないので、被処理
基板の電位差の増大には上限があるといえる。被処理基
板と静電吸着電極の距離、すなわち被処理基板の電位の
みを調節することでDC放電の発生を操作するのが、実
用上、困難な場合がある。このような場合に、DC放電
の発生を操作するには、パッセンの法則にしたがって、
被処理基板周辺に存在するガスの圧力を制御することが
もっとも簡単といえる。被処理基板周辺に存在するガス
とは、被処理基板近傍でDC放電を発生させる雰囲気を
形成できるガスであればなんでもよい。たとえば、窒
素、酸素、水素、イオウ、塩素またはフッ素原子のうち
少なくとも1種を含む混合ガス等、処理用ガス、基板処
理後に残った残留ガス、または、残留ガスを追い出すた
めのパ−ジガスでもよい。ガスの圧力を制御する観点か
ら、真空容器に導入されるガス、すなわち処理用ガスま
たはパージガスを使用するのがもっともよい。Since the distance between the substrate to be processed and the electrostatic attraction electrode can be set only to the extent that a minute gap is formed, it can be said that the increase in the potential difference of the substrate to be processed has an upper limit. It may be practically difficult to control the generation of DC discharge by adjusting the distance between the substrate to be processed and the electrostatic attraction electrode, that is, only the potential of the substrate to be processed. In such a case, in order to control the generation of the DC discharge, according to Passen's law,
It can be said that it is easiest to control the pressure of the gas existing around the substrate to be processed. The gas existing around the substrate to be processed may be any gas as long as it can form an atmosphere in which DC discharge is generated near the substrate to be processed. For example, it may be a processing gas such as a mixed gas containing at least one of nitrogen, oxygen, hydrogen, sulfur, chlorine or fluorine atoms, a residual gas left after the substrate processing, or a purge gas for expelling the residual gas. . From the viewpoint of controlling the gas pressure, it is best to use the gas introduced into the vacuum vessel, that is, the processing gas or the purge gas.
【0034】発明者らは、静電吸着のために静電吸着電
極に印加する電圧と無関係に、8インチ半導体ウエハと
静電吸着電極間が約0.1mmでは、アースに対するウ
エハの電位差は約4,000V、約1mmでは約40,
000Vであることを発見した。また、この電位差の範
囲で、N2 ガスの圧力を0.1Paから500Paに設
定するとDC放電が発生することを発見した。後述する
ように、発明者らは、この圧力範囲で10秒以内に被処
理基板を離脱することができた。しかも、被処理基板の
残留電荷が完全には消失されない段階でも、被処理基板
の表面電位が放電維持電位以下であれば、ピンで引続き
徐々に被処理基板を持ち上げることにより、静電吸着電
極の吸着面から被処理基板を引き離すことができた。発
明者らは、8インチの半導体ウエハの表面電位が220
Vに達したときに静電吸着電極から引き離すという条件
で2,500枚の半導体ウエハを連続して離脱しても、
半導体ウエハに損傷なく、正確に離脱ができたことを確
認した。表1は、リアクティブイオンエッチング装置中
で静電吸着電極に−1000Vの直流電圧を印加して静
電吸着電極の吸着面に固定した半導体ウエハにエッチン
グ処理をしたあとに3通りの方法で基板を離脱したとき
の基板の表面電位をしめす。直流電圧印可停止後、
(1)静電吸着電極の吸着面からピンを突き出して半導
体ウエハを持ち上げる瞬間に、窒素ガスをウエハの置か
れた真空容器内に導入し、圧力20Paに保持したま
ま、半導体ウエハを静電吸着電極から離脱させた方法、
(2)真空容器内の圧力が0.05Paの状態で、ピン
による半導体ウエハの持ち上げのみで強制的に静電吸着
電極から離脱させた方法、(3)ピンで半導体ウエハを
持ち上げる前に、半導体ウエハの置かれた真空容器内に
窒素ガスを導入して圧力を20Paに設定し1分間放置
後、窒素ガスを排気してから(0.05Pa)ピンで半
導体ウエハを持ち上げて電極から離脱させた方法につい
て半導体ウエハの表面電位を比較したものである。各場
合とも、表面電位測定時の半導体ウエハの位置は、静電
吸着電極の吸着面から10mmである。ここで、半導体
ウエハの表面電位は、トレック社の静電気測定表面電位
計モデル344(TREK Inc. Electrostaticvoltmeter mo
del 344)を用いて測定した。ちなみに、直流電圧印加
停止後、半導体ウエハが静電吸着電極に載置されたまま
での半導体ウエハの表面電位は、370Vであった。The inventors have found that, regardless of the voltage applied to the electrostatic attraction electrode for electrostatic attraction, when the distance between the 8-inch semiconductor wafer and the electrostatic attraction electrode is about 0.1 mm, the potential difference of the wafer with respect to the ground is about. 4,000V, about 40mm at about 1mm,
It was found to be 000V. Further, it was discovered that when the pressure of N 2 gas was set from 0.1 Pa to 500 Pa within this potential difference range, DC discharge occurred. As will be described later, the inventors were able to separate the substrate to be processed within 10 seconds within this pressure range. Moreover, even when the residual charge of the substrate to be processed is not completely lost, if the surface potential of the substrate to be processed is lower than the discharge sustaining potential, the substrate to be processed is gradually lifted up by the pin to gradually remove the electrostatic adsorption electrode. The substrate to be processed could be separated from the suction surface. The inventors have found that the surface potential of an 8-inch semiconductor wafer is 220
Even if 2,500 semiconductor wafers are continuously separated under the condition that they are separated from the electrostatic attraction electrode when reaching V,
It was confirmed that the semiconductor wafer could be separated accurately without damage. Table 1 shows that after applying a DC voltage of −1000 V to the electrostatic adsorption electrode in the reactive ion etching apparatus to etch the semiconductor wafer fixed on the adsorption surface of the electrostatic adsorption electrode, the substrate is divided into three types by the following three methods. Shows the surface potential of the substrate when it is released. After applying DC voltage,
(1) Nitrogen gas is introduced into the vacuum container where the wafer is placed at the moment when the pins are ejected from the adsorption surface of the electrostatic adsorption electrode to lift the semiconductor wafer, and the semiconductor wafer is electrostatically adsorbed while the pressure is kept at 20 Pa. Method of detaching from the electrode,
(2) A method in which the pressure inside the vacuum container is 0.05 Pa, the semiconductor wafer is forcibly detached from the electrostatic attraction electrode only by lifting the semiconductor wafer by the pin, and (3) before the semiconductor wafer is lifted by the pin, the semiconductor Nitrogen gas was introduced into the vacuum container in which the wafer was placed, the pressure was set to 20 Pa, and after leaving it for 1 minute, the nitrogen gas was exhausted, and then the semiconductor wafer was lifted with a (0.05 Pa) pin to separate it from the electrode. The method is a comparison of the surface potentials of semiconductor wafers. In each case, the position of the semiconductor wafer at the time of measuring the surface potential is 10 mm from the attraction surface of the electrostatic attraction electrode. Here, the surface potential of the semiconductor wafer is the electrostatic measurement surface potential meter model 344 (TREK Inc. Electrostatic voltmeter
del 344). Incidentally, after the application of the DC voltage was stopped, the surface potential of the semiconductor wafer with the semiconductor wafer still mounted on the electrostatic attraction electrode was 370V.
【0035】[0035]
【表1】 [Table 1]
【0036】(1)の方法で離脱させた半導体ウエハの
表面電位は、(2)および(3)の方法で離脱させた半
導体ウエハの表面電位に比べて非常に小さい。このこと
は、半導体ウエハ近傍でDC放電が発生したことで、半
導体ウエハに帯電した静電気量がかなり失っているとい
える。たぶん、半導体ウエハと静電吸着電極の距離と窒
素ガスの圧力から、半導体ウエハとアースされた部品、
たとえば、対向電極または真空容器の壁面との間で放電
が発生していると推測できる。そして放電により帯電し
たガス分子が、帯電していた半導体ウエハを除電したこ
とを示している。(2)の方法で離脱された半導体ウエ
ハの表面電位から半導体ウエハにかなりの静電気量が残
っているといえる。(3)の方法で離脱された半導体ウ
エハの表面電位は(2)の方法での表面電位とほとんど
同じである。単に真空容器にガスを導入して排出しただ
けでは、帯電した半導体ウエハの電荷を十分に除電でき
ないことを示している。なお、(2)および(3)の方
法で離脱された半導体ウエハの表面電位は、半導体ウエ
ハが静電吸着電極に載置されたままでの表面電位(37
0V)および(c)式から予想される電位よりも低くな
っている。これは、浮遊電気容量の影響だといえる。The surface potential of the semiconductor wafer separated by the method (1) is much smaller than the surface potential of the semiconductor wafer separated by the methods (2) and (3). This means that the amount of static electricity charged on the semiconductor wafer is considerably lost due to the occurrence of DC discharge in the vicinity of the semiconductor wafer. Perhaps, from the distance between the semiconductor wafer and the electrostatic attraction electrode and the pressure of nitrogen gas, the semiconductor wafer and the grounded component,
For example, it can be inferred that discharge is occurring between the counter electrode and the wall surface of the vacuum container. Then, it is shown that the gas molecules charged by the discharge have discharged the charged semiconductor wafer. It can be said that a considerable amount of static electricity remains on the semiconductor wafer from the surface potential of the semiconductor wafer separated by the method (2). The surface potential of the semiconductor wafer separated by the method (3) is almost the same as the surface potential by the method (2). This indicates that the charge of the charged semiconductor wafer cannot be sufficiently removed by simply introducing and discharging the gas in the vacuum container. The surface potential of the semiconductor wafer separated by the methods (2) and (3) is the surface potential (37) of the semiconductor wafer while it is mounted on the electrostatic adsorption electrode.
0 V) and lower than the potential expected from the equation (c). This can be said to be the effect of stray capacitance.
【0037】これらの結果から、静電吸着電極から半導
体ウエハを引き離す際に、被処理基板近傍を放電発生の
雰囲気とするために真空容器にガス(雰囲気ガス)を充
てんしておくこと或いは充てんすることが重要であると
いえる。したがって、本発明の離脱方法を実施する基板
離脱機構には、雰囲気ガスの導入、ピンの突出、圧力調
整を順次稼働させるためのシーケンサを備えておくこと
が望ましい。From these results, when the semiconductor wafer is separated from the electrostatic attraction electrode, the vacuum container is filled or filled with gas (atmosphere gas) so that the vicinity of the substrate to be processed has an atmosphere for generating discharge. Can be said to be important. Therefore, it is desirable that the substrate detaching mechanism for carrying out the detaching method of the present invention is provided with a sequencer for sequentially operating the introduction of the atmospheric gas, the protrusion of the pins, and the pressure adjustment.
【0038】表2は、リアクティブイオンエッチング装
置中で静電吸着電極に−1000Vの直流電圧を印加す
ることにより固定した半導体ウエハにエッチング処理を
した後に、ピンで半導体ウエハを持ち上げる瞬間に窒素
ガスを半導体ウエハの置かれたチャンバー内に導入し、
(1)0.05Pa、(2)0.1Pa、(3)10P
a、(4)50Pa、(5)500Pa、(6)600
Paの圧力で真空容器内を充てんした場合に、表面電位
が100V以下になるのに要する時間を示したものであ
る。静電吸着電極の吸着面から突き出したピンの高さ
は、約0.1mmから約1mmであった。Table 2 shows that after etching the semiconductor wafer fixed by applying a DC voltage of -1000 V to the electrostatic adsorption electrode in the reactive ion etching apparatus, the nitrogen gas was lifted at the moment when the semiconductor wafer was lifted by the pins. Is introduced into the chamber in which the semiconductor wafer is placed,
(1) 0.05Pa, (2) 0.1Pa, (3) 10P
a, (4) 50 Pa, (5) 500 Pa, (6) 600
It shows the time required for the surface potential to reach 100 V or less when the vacuum container is filled with a pressure of Pa. The height of the pin protruding from the attraction surface of the electrostatic attraction electrode was about 0.1 mm to about 1 mm.
【0039】[0039]
【表2】 [Table 2]
【0040】圧力が0.1〜500Paで、いずれも1
0秒以内で100V以下に達している。つまり、被処理
基板と静電吸着電極との間隔が約0.1mmから約1m
mのもと0.1〜500Paの圧力範囲で、半導体ウエ
ハと静電吸着電極との間で雰囲気ガス(N2 ガス)が放
電が発生したことをしめしている。The pressure is 0.1 to 500 Pa, and both are 1
It reached 100V or less within 0 seconds. That is, the distance between the substrate to be processed and the electrostatic attraction electrode is about 0.1 mm to about 1 m.
It is shown that discharge of atmospheric gas (N 2 gas) occurred between the semiconductor wafer and the electrostatic adsorption electrode within a pressure range of 0.1 to 500 Pa under m.
【0041】[0041]
【実施例】図1は本発明の第1実施例の構成図を示す。
図中、1は真空槽10内にガスを導入する系のガスパイ
プ、2は静電吸着電極、3は静電吸着電極2の表面を覆
った誘電体シート、4は静電吸着電極2に直流電圧を印
加するための直流電源、5はイオンエッチングなどを行
うための被処理基板、6は電極保持体、7は自動圧力制
御機構(Auto Pressure Controller)、7aは流量制御
弁、7bは排気系(図はターボモレキュラーポンプとロ
ータリーポンプで構成した例を示す。)、8はプラズマ
源、9は静電吸着電極2内に埋設されたリフトピンを示
す。リフトピン9は軸受11a、11bで支持された駆
動軸13を介して、駆動部材13aの昇降により誘電体
シート3の表面から突出、没入するようになっている。
12はフレームで、駆動部材13aを昇降させる駆動機
構(図示していない)が設置してある。1 is a block diagram of the first embodiment of the present invention.
In the figure, 1 is a gas pipe for introducing gas into the vacuum chamber 10, 2 is an electrostatic attraction electrode, 3 is a dielectric sheet covering the surface of the electrostatic attraction electrode 2, and 4 is a direct current to the electrostatic attraction electrode 2. Direct current power source for applying voltage, 5 substrate to be processed for performing ion etching, 6 electrode holder, 7 automatic pressure control mechanism (Auto Pressure Controller), 7a flow control valve, 7b exhaust system (The figure shows an example constituted by a turbo molecular pump and a rotary pump.), 8 is a plasma source, and 9 is a lift pin embedded in the electrostatic attraction electrode 2. The lift pin 9 is adapted to project and retract from the surface of the dielectric sheet 3 when the drive member 13a is moved up and down via the drive shaft 13 supported by the bearings 11a and 11b.
A frame 12 is provided with a drive mechanism (not shown) for moving the drive member 13a up and down.
【0042】図1において、被処理基板5をエッチング
加工する場合、被処理基板5を図示されない搬送手段を
用いて誘電体シート3を介して静電吸着電極2上に設置
し、次に直流電源4より静電吸着電極2に直流電圧を印
加する。同時に真空槽10にガス導入系のガスパイプ1
より塩素ガスを導入し、自動圧力制御機構7により所定
の圧力(約0.5Pa)にする。次いで、プラズマ源8
によりプラズマを発生させる。プラズマにより静電吸着
電極2、直流電源4を含む直流回路が形成され、被処理
基板5は静電吸着電極2に固定されると共に、被処理基
板5の表面がエッチング加工される。処理終了後、ガス
パイプ1より窒素ガスを導入し、自動圧力制御機構7で
圧力制御(約2Pa)を行ないつつ、プラズマ源8およ
び直流電源4をOFFとし、静電吸着電極2内に埋設さ
れたリフトピン9を誘電体シート3の表面から0.5m
m程度突出させる。被処理基板5が静電吸着電極2より
離脱しはじめたら、リフトピン9を更に突出させ、被処
理基板5を完全に離脱させる。リフトピン9の突出開始
から離脱完了までに要する時間は、約3秒であった。In FIG. 1, when etching the substrate 5 to be processed, the substrate 5 to be processed is placed on the electrostatic attraction electrode 2 via the dielectric sheet 3 using a transporting means (not shown), and then a DC power source is used. A DC voltage is applied to the electrostatic attraction electrode 2 from 4. At the same time, a gas pipe 1 for introducing gas into the vacuum chamber 10
Chlorine gas is further introduced, and a predetermined pressure (about 0.5 Pa) is set by the automatic pressure control mechanism 7. Then, the plasma source 8
To generate plasma. A direct current circuit including the electrostatic attraction electrode 2 and the direct current power source 4 is formed by the plasma, the target substrate 5 is fixed to the electrostatic attracting electrode 2, and the surface of the target substrate 5 is etched. After completion of the treatment, nitrogen gas was introduced from the gas pipe 1, the pressure control (about 2 Pa) was performed by the automatic pressure control mechanism 7, the plasma source 8 and the DC power supply 4 were turned off, and the gas was buried in the electrostatic adsorption electrode 2. Lift pin 9 from the surface of dielectric sheet 3 by 0.5 m
Protrude about m. When the substrate 5 to be processed begins to separate from the electrostatic attraction electrode 2, the lift pins 9 are further projected to completely separate the substrate 5 to be processed. The time required from the start of the protrusion of the lift pin 9 to the completion of the separation was about 3 seconds.
【0043】図2は本発明の第2実施例の構成図、詳し
くは平行平板型反応性イオンエッチング(RIE)装置
に本発明を応用した場合の構成図である。14が高周波
電源、15が接地電極であり、他の部分は図1の実施例
と同様の構成である。FIG. 2 is a block diagram of a second embodiment of the present invention, more specifically, a block diagram when the present invention is applied to a parallel plate type reactive ion etching (RIE) apparatus. Reference numeral 14 is a high frequency power source, 15 is a ground electrode, and the other parts have the same structure as the embodiment of FIG.
【0044】図2において、被処理基板5を加工する場
合、被処理基板5を図示されない搬送手段を用いて誘電
体膜3を介して静電吸着電極2上に設置し、次に直流電
源4より静電吸着電極2に直流電圧を印加する。同時に
真空槽10にガス導入系を構成したガスパイプ1よりプ
ロセスガス(CF4 +O2 )を導入し、自動圧力制御機
構7により所定の圧力(約10Pa)にする。次いで、
高周波電源14より静電吸着電極2に高周波電力を供給
し、静電吸着電極2と接地電極15との間に反応性ガス
プラズマを発生させる。プラズマにより静電吸着電極
2、直流電源4を含む直流回路が形成され、被処理基板
5は静電吸着電極2に固定されると共に、被処理基板5
の表面がエッチング加工される。処理終了後も引続きガ
スパイプ1より前記プロセスガスを導入し、自動圧力制
御機構で圧力制御(約10Pa)を行ないつつ、高周波
電源14および直流電源4をOFFし、静電吸着電極2
内に埋設されたリフトピン9を誘電体シート3の表面か
ら0.5mm程度突出させる。被処理基板5が静電吸着
電極2より離脱しはじめたら、リフトピン9を更に突出
させ、被処理基板5を完全に離脱させる。この場合のリ
フトピン9の突出開始から離脱完了までに要する時間は
約2秒であった。In FIG. 2, when the substrate 5 to be processed is processed, the substrate 5 to be processed is placed on the electrostatic attraction electrode 2 via the dielectric film 3 by using a transfer means (not shown), and then the DC power source 4 is used. Further, a DC voltage is applied to the electrostatic attraction electrode 2. At the same time, the process gas (CF 4 + O 2 ) is introduced into the vacuum chamber 10 from the gas pipe 1 which constitutes the gas introduction system, and the automatic pressure control mechanism 7 brings the process gas to a predetermined pressure (about 10 Pa). Then
A high frequency power is supplied from the high frequency power supply 14 to the electrostatic attraction electrode 2 to generate a reactive gas plasma between the electrostatic attraction electrode 2 and the ground electrode 15. A direct current circuit including the electrostatic attraction electrode 2 and the direct current power supply 4 is formed by the plasma, and the substrate 5 to be processed is fixed to the electrostatic attraction electrode 2 and the substrate 5 to be processed 5
The surface of is etched. After the processing is completed, the process gas is continuously introduced through the gas pipe 1, and the high-frequency power source 14 and the direct-current power source 4 are turned off while the pressure control (about 10 Pa) is performed by the automatic pressure control mechanism, and the electrostatic attraction electrode 2
The lift pins 9 embedded inside are projected from the surface of the dielectric sheet 3 by about 0.5 mm. When the substrate 5 to be processed begins to separate from the electrostatic attraction electrode 2, the lift pins 9 are further projected to completely separate the substrate 5 to be processed. In this case, the time required from the start of the protrusion of the lift pin 9 to the completion of the separation was about 2 seconds.
【0045】前記エッチング処理の終了後、導入するガ
スをアルゴンに切換えて、真空槽10内の圧力を10P
aに維持した状態で、前記と同様の離脱動作を行ったと
ころ、リフトピン9の突出開始から離脱完了までの時間
を約1秒とすることができた。After the etching process is completed, the gas to be introduced is switched to argon and the pressure in the vacuum chamber 10 is set to 10 P.
When the same detaching operation as described above was performed in the state of being maintained at a, the time from the start of protrusion of the lift pins 9 to the completion of detachment could be about 1 second.
【0046】尚、上記の各実施例では、真空槽10を被
処理基板5の加工処理部を構成するチャンバーと、被処
理基板の離脱動作が行なわれるチャンバーに共用してい
るが、これらを別個として、被処理基板5を電極2と共
に、離脱動作が行なわれる別のチャンバーに移送し、該
部で離脱操作を行う構成とすることもできる。In each of the above embodiments, the vacuum chamber 10 is shared by the chamber constituting the processing portion of the substrate 5 to be processed and the chamber for separating the substrate to be processed. Alternatively, the substrate 5 to be processed may be transferred together with the electrode 2 to another chamber where the detaching operation is performed, and the detaching operation may be performed in this part.
【0047】また、ガスパイプ1はプロセスガスの導入
系と被処理基板5の離脱の際に導入するガスの導入系を
共通としたが、別個とすることもできる。更には、離脱
の際に導入するガスの導入系を、チャンバーのベント用
として設けられる空気又は窒素ガスの導入系と共通にす
ることもできる。第1実施例のように、プロセスガスと
離脱時のガスが異なる場合、別個の導入系とした方が操
作性は良くなるであろう。Further, the gas pipe 1 has a common system for introducing the process gas and a system for introducing the gas to be introduced when the substrate 5 to be processed is separated, but they may be separate systems. Furthermore, the gas introduction system introduced at the time of separation can be made common with the air or nitrogen gas introduction system provided for venting the chamber. When the process gas and the gas at the time of desorption are different as in the first embodiment, the operability may be improved by using separate introduction systems.
【0048】図3は第3実施例の構成図を示す。詳しく
はマルチチャンバエッチングシステム(ANELVA−
4100)の平行平板形反応性エッチング処理用にモジ
ュ−ル化されたチャンバ(真空容器)に組み込まれた基
板離脱機構の図である。前記の実施例と同様に、1は真
空槽10内にガスを導入するパイプ、1a、1bはバル
ブ、20はエッチングガス供給源、21は雰囲気ガス供
給用源を示す。2は静電吸着電極、3は静電吸着電極2
の表面を覆った誘電体シ−トで基板の吸着面を構成して
いる。4は静電吸着電極2に直流電圧を印加するための
直流電源、5は8インチの半導体ウエハ(被処理基
板)、6は保持体、14が高周波電源、15が接地電極
を示す。7は自動圧力制御機構(Auto Pressure Contro
ller)、7aは排気用バルブ、7bはターボモレキュラ
ーポンプとロータリーポンプで構成した排気系を示す。
自動圧力制御機構7は、バルブ7aの開口の度合いを調
整して真空容器内の圧力を調整する。9は静電吸着電極
2内に設置されたリフトピンを示す。4つのリフトピン
で半導体ウエハ5を持ち上げるもので、被処理基板に機
械的離脱力を付与する手段を構成している。4つのリフ
トピンは、図4に示されるように半導体ウエハ5の直径
よりも短い円の円周上に等間隔で設けられている(第
1、第2実施例も同様である。)。リフトピン9は軸受
11a、11bで支持された駆動軸13に連結されてお
り、駆動部材13aの昇降により誘電体シ−ト3の表面
から突出、没入するようになっている。12は真空槽1
0の底部に設置したフレームで、駆動部材13aを昇降
させる駆動機構22が設置される。駆動機構22は、半
導体ウエハ5と静電吸着電極2間に微間隙を形成する際
に、リフトピン9の吸着面から突き出す高さを、半導体
ウエハ5を破損しない程度の高さに調整できる構成とし
てある。具体的には、リフトピン9の突き出す高さを
0.1mmから1mm程度に調整可能としてある。23
は、シ−ケンサを示す。シ−ケンサ23は、バルブ1
a、1bの開閉、自動圧力制御機構7の起動および駆動
機構23の起動を制御する。FIG. 3 shows a block diagram of the third embodiment. For details, see Multi-chamber Etching System (ANELVA-
4100) is a diagram of a substrate release mechanism incorporated in a chamber (vacuum container) modularized for the parallel plate reactive etching process of FIG. Similar to the above-described embodiment, 1 is a pipe for introducing gas into the vacuum chamber 10, 1a and 1b are valves, 20 is an etching gas supply source, and 21 is an atmosphere gas supply source. 2 is an electrostatic adsorption electrode, 3 is an electrostatic adsorption electrode 2
The dielectric sheet covering the surface of the substrate constitutes the attracting surface of the substrate. Reference numeral 4 is a DC power source for applying a DC voltage to the electrostatic attraction electrode 2, 5 is an 8-inch semiconductor wafer (substrate to be processed), 6 is a holder, 14 is a high frequency power source, and 15 is a ground electrode. 7 is an automatic pressure control mechanism.
ller), 7a is an exhaust valve, and 7b is an exhaust system composed of a turbo molecular pump and a rotary pump.
The automatic pressure control mechanism 7 adjusts the degree of opening of the valve 7a to adjust the pressure inside the vacuum container. Reference numeral 9 denotes a lift pin installed in the electrostatic attraction electrode 2. The semiconductor wafer 5 is lifted by the four lift pins, and constitutes a means for applying a mechanical detaching force to the substrate to be processed. As shown in FIG. 4, the four lift pins are provided at equal intervals on the circumference of a circle shorter than the diameter of the semiconductor wafer 5 (the same applies to the first and second embodiments). The lift pin 9 is connected to a drive shaft 13 supported by bearings 11a and 11b, and is configured to project and retract from the surface of the dielectric sheet 3 when the drive member 13a moves up and down. 12 is a vacuum tank 1
A drive mechanism 22 for raising and lowering the drive member 13a is installed on the frame installed at the bottom of 0. The drive mechanism 22 has a configuration in which the height of the lift pin 9 protruding from the suction surface when the fine gap is formed between the semiconductor wafer 5 and the electrostatic suction electrode 2 is adjusted to a height that does not damage the semiconductor wafer 5. is there. Specifically, the protruding height of the lift pin 9 can be adjusted to about 0.1 mm to 1 mm. 23
Indicates a sequencer. The sequencer 23 is a valve 1
The opening and closing of a, 1b, the activation of the automatic pressure control mechanism 7 and the activation of the drive mechanism 23 are controlled.
【0049】前記の平行平板形反応性エッチング処理用
にモジュ−ル化されたチャンバに組み込まれた基板離脱
機構を用いた基板離脱動作を説明する。The substrate detaching operation using the substrate detaching mechanism incorporated in the chamber modularized for the parallel plate type reactive etching process will be described.
【0050】半導体ウエハ5を図示されない搬送ロボッ
トを用いて、静電吸着電極2を覆った誘電体シ−ト3で
なる吸着面上に載置する。次に直流電源4より静電吸着
電極2に直流電圧(例えば−1000V)を印加する。
バルブ1aを開いて真空槽10にパイプ1よりエッチン
グガス(CF4 +O2 )を導入する。エッチングガスの
圧力を自動圧力制御機構7により約10Paに設定す
る。次いで、高周波電源14より静電吸着電極2に高周
波電力を供給し、静電吸着電極2と接地電極15との間
に反応性プラズマを発生させる。プラズマにより静電吸
着電極2、直流電源4を含む直流回路が形成され、半導
体ウエハ5は静電吸着電極2に固定されると共に、半導
体ウエハ5の表面がエッチングされる。所定時間の経過
後、高周波電源14および直流電源4をOFFにしてエ
ッチング処理を終了する。処理終了後も引続きバルブ1
aを開いたまま、ガスパイプ1よりエッチングガスCF
4 +O2 (90/10sccm)を導入しながら、シ−
ケンサ23が駆動機構を起動させて、静電吸着電極2内
に埋設されたリフトピン9を誘電体シ−ト3の表面から
0.5mm程度突出させる。その一方で、シ−ケンサ2
3が自動圧力制御機構7を起動させてエッチングガスの
圧力を約10Paに設定させる。放電による除電作用の
結果、半導体ウエハ5が静電吸着電極2より離脱しはじ
めたら、リフトピン9を更に突出させ、半導体ウエハ5
を完全に離脱させる。この場合のリフトピン9の突出開
始から離脱完了まで約2秒を要した。この実施例でも、
離脱の際に半導体ウエハ5と静電吸着電極2で放電を発
生させるための雰囲気ガスとしては第2実施例と同様
に、エッチングガスを使用したものである。The semiconductor wafer 5 is placed on the attraction surface made of the dielectric sheet 3 covering the electrostatic attraction electrode 2 by using a transfer robot (not shown). Next, a DC voltage (for example, −1000 V) is applied to the electrostatic attraction electrode 2 from the DC power supply 4.
The valve 1a is opened, and the etching gas (CF 4 + O 2 ) is introduced into the vacuum chamber 10 through the pipe 1. The pressure of the etching gas is set to about 10 Pa by the automatic pressure control mechanism 7. Then, high frequency power is supplied from the high frequency power supply 14 to the electrostatic attraction electrode 2 to generate reactive plasma between the electrostatic attraction electrode 2 and the ground electrode 15. A direct current circuit including the electrostatic attraction electrode 2 and the direct current power source 4 is formed by the plasma, the semiconductor wafer 5 is fixed to the electrostatic attraction electrode 2, and the surface of the semiconductor wafer 5 is etched. After the elapse of a predetermined time, the high frequency power supply 14 and the direct current power supply 4 are turned off to end the etching process. Valve 1 continues after processing
Etching gas CF from gas pipe 1 with a open
While introducing 4 + O 2 (90/10 sccm),
The counter 23 activates the drive mechanism to cause the lift pin 9 embedded in the electrostatic attraction electrode 2 to protrude from the surface of the dielectric sheet 3 by about 0.5 mm. On the other hand, Sequencer 2
3 activates the automatic pressure control mechanism 7 to set the pressure of the etching gas to about 10 Pa. When the semiconductor wafer 5 starts to separate from the electrostatic attraction electrode 2 as a result of the static elimination action by the discharge, the lift pins 9 are further projected to make the semiconductor wafer 5
To leave completely. In this case, it took about 2 seconds from the start of the protrusion of the lift pin 9 to the completion of the separation. Also in this example,
As in the second embodiment, an etching gas is used as an atmosphere gas for generating a discharge between the semiconductor wafer 5 and the electrostatic attraction electrode 2 at the time of separation.
【0051】第4実施例として、図3の機構において、
エッチングガスおよび雰囲気ガスともにCF4 +CHF
3 (150/50sccm)を用いた。雰囲気ガスの圧
力を20Paに設定して、第3実施例と同じ離脱動作を
行ったところ、リフトピン9の突出開始から離脱完了ま
でに約1秒を要した。As a fourth embodiment, in the mechanism of FIG.
CF 4 + CHF for both etching gas and atmosphere gas
3 (150/50 sccm) was used. When the pressure of the atmospheric gas was set to 20 Pa and the same detaching operation as in the third embodiment was performed, it took about 1 second from the start of the protrusion of the lift pin 9 to the completion of the detachment.
【0052】第5実施例として、第3実施例でのエッチ
ング処理の終了後、シ−ケンサ23によりバルブ1aを
閉めてから、バルブ1bを開けてアルゴンガス(雰囲気
ガス)(200sccm)を真空容器10内に導入し
た。その導入と同時にシ−ケンサ23が駆動機構を起動
させて、リフトピン9を0.5mm程度突出させる。そ
の一方で、シ−ケンサ23が自動圧力制御機構7を起動
させてアルゴンガスの圧力を約10Paに設定した。リ
フトピン9の突出開始から離脱完了までが約1秒を要し
た。As a fifth embodiment, after the etching process in the third embodiment is completed, the valve 1a is closed by the sequencer 23, and then the valve 1b is opened to supply the argon gas (atmosphere gas) (200 sccm) to the vacuum container. Introduced in 10. Simultaneously with the introduction, the sequencer 23 activates the drive mechanism to cause the lift pin 9 to project by about 0.5 mm. On the other hand, the sequencer 23 activated the automatic pressure control mechanism 7 to set the pressure of the argon gas to about 10 Pa. It took about 1 second from the start of the protrusion of the lift pin 9 to the completion of the separation.
【0053】第6実施例として、第3実施例でのエッチ
ング処理の終了後、雰囲気ガスとしてN2 (200sc
cm)を用いた。雰囲気ガスの圧力を20Paに設定し
て、第3実施例と同じ離脱動作を行ったところ、リフト
ピン9の突出開始から離脱完了までが約1秒を要した。As a sixth embodiment, after completion of the etching treatment in the third embodiment, N 2 (200 sc
cm) was used. When the pressure of the atmospheric gas was set to 20 Pa and the same detaching operation as in the third embodiment was performed, it took about 1 second from the start of protrusion of the lift pin 9 to the completion of detachment.
【0054】第7実施例としてANELVA−4100
のヘリコン波エッチング処理用にモジュ−ル化されたチ
ャンバ(ヘリコン波プラズマ発生装置が搭載されてい
る)に組み込まれた基板離脱機構での基板離脱動作を説
明する。ここで、基板離脱機構は、図3における平行平
板形反応性エッチング処理用にモジュ−ル化されたチャ
ンバに組み込まれた基板離脱機構と全く同じである。ヘ
リコン波プラズマ発生装置は、米国特許4,990,2
29および5,122,251に記載されている。エッ
チングガスとして塩素ガスをチャンバに導入し、ヘリコ
ン波プラズマを発生させてエッチング処理を行う。ヘリ
コン波プラズマ発生装置および直流電源4をOFFにし
て処理を終了する。その後、雰囲気ガスとして窒素ガス
(200sccm)をチャンバ内に導入し、自動圧力制
御機構7で約2Paに設定する。それと同時に、静電吸
着電極2内に埋設されたリフトピン9を誘電体シ−ト3
の表面から0.5mm程度突出させる。半導体ウエハ5
が電極2より離脱しはじめたら、リフトピン9を更に突
出させ、半導体ウエハ5を完全に離脱させる。リフトピ
ン9の突出開始から離脱完了までに要する時間は、約3
秒であった。As a seventh embodiment, ANELVA-4100
The substrate detaching operation by the substrate detaching mechanism incorporated in the chamber (the helicon wave plasma generator is mounted) that is modularized for the helicon wave etching process will be described. Here, the substrate separating mechanism is exactly the same as the substrate separating mechanism incorporated in the chamber modularized for the parallel plate type reactive etching process in FIG. A helicon wave plasma generator is disclosed in US Pat. No. 4,990,2.
29 and 5,122,251. Chlorine gas is introduced into the chamber as an etching gas and helicon wave plasma is generated to perform the etching process. The helicon wave plasma generator and the DC power supply 4 are turned off, and the process is terminated. Then, nitrogen gas (200 sccm) is introduced into the chamber as an atmosphere gas, and the pressure is set to about 2 Pa by the automatic pressure control mechanism 7. At the same time, the lift pin 9 embedded in the electrostatic attraction electrode 2 is attached to the dielectric sheet 3
About 0.5 mm from the surface. Semiconductor wafer 5
When the wafer starts to separate from the electrode 2, the lift pin 9 is further projected to completely separate the semiconductor wafer 5. The time required from the start of the protrusion of the lift pin 9 to the completion of the separation is about 3
It was seconds.
【0055】離脱の際に充てんするガスを空気としても
よい。この場合、真空容器(チャンバー)10に別途設
けたベント用バルブ(図示していない)を開けて空気を
チャンバ内に導入する。The gas filled at the time of separation may be air. In this case, a vent valve (not shown) separately provided in the vacuum container (chamber) 10 is opened to introduce air into the chamber.
【0056】上記各実施例ではプラズマエッチング処理
の場合を説明したが、被処理基板を静電吸着するように
した、プラズマCVD装置、スパッタリング装置、プラ
ズマアッシング装置においても本発明の基板離脱機構を
組み込んだプラズマ処理装置を構成できるとともに本発
明の離脱方法が実施可能である。また、各実施例では、
被処理基板(半導体ウエハ)の周辺の雰囲気中に存在す
るガスの圧力を設定した後に、微間隙、即ち被処理基板
と静電吸着電極間の間隔を形成したが、微間隙を形成し
た後に、雰囲気ガスの圧力を、放電開始圧力に調整する
ようにすることも可能である。In each of the above embodiments, the case of the plasma etching process is explained, but the substrate detaching mechanism of the present invention is also incorporated in the plasma CVD device, the sputtering device and the plasma ashing device which electrostatically attract the substrate to be processed. The plasma processing apparatus can be configured and the detachment method of the present invention can be implemented. Also, in each example,
After setting the pressure of the gas existing in the atmosphere around the substrate to be processed (semiconductor wafer), a small gap, that is, the space between the substrate to be processed and the electrostatic attraction electrode was formed. It is also possible to adjust the pressure of the atmospheric gas to the discharge starting pressure.
【0057】図5は、機械的離脱力付与手段の別の実施
例で、吸着面を構成した誘電体シート3の中央部に、円
形台24を設けたものである。円形台24は、駆動軸1
3と連結されて突没自在としてあり、没入時には、上面
が吸着面と面一となるようにしてある。この円形台24
による機械的離脱力付与手段によっても、被処理基板と
吸着面の間に微間隙を形成することが可能であり、前記
実施例と同様にして、被処理基板の離脱を行うことがで
きる。FIG. 5 shows another embodiment of the mechanical separating force applying means, in which a circular base 24 is provided at the center of the dielectric sheet 3 constituting the suction surface. The circular base 24 is the drive shaft 1
It is connected to 3 so that it can be projected and retracted, and the upper surface thereof is flush with the suction surface when retracted. This round table 24
The mechanical separation force imparting means by means of can also form a fine gap between the substrate to be processed and the suction surface, and the substrate to be processed can be separated in the same manner as in the above-mentioned embodiment.
【0058】被処理基板5の離脱の際、導入したガスの
圧力は2Pa、10Pa、および20Paの場合につい
て説明したが、およそ0.1Pa〜500Paの範囲で
実用上十分な残留電荷の消失効果を得ることができる。
圧力を高くするに従って消失速度が速まり、離脱時間の
短縮効果があるが、圧力が高くなりすぎると残留電荷の
消失効果は再び減じる。The case where the pressure of the gas introduced at the time of detaching the substrate 5 to be processed is 2 Pa, 10 Pa, and 20 Pa has been described, but in the range of approximately 0.1 Pa to 500 Pa, a practically sufficient residual charge disappearing effect is obtained. Obtainable.
The higher the pressure is, the faster the disappearance speed is, and the effect of shortening the detachment time is obtained. However, when the pressure is too high, the effect of disappearing the residual charge is reduced again.
【0059】[0059]
【発明の効果】以上に説明したように、本発明によれ
ば、減圧下で被処理基板を静電吸着により電極に固定し
て被処理基板の加工を行うような装置において、静電吸
着電極からの被処理基板の離脱を迅速かつ容易に行わし
める効果がある。また、残留する静電吸着力が原因とし
て起こる基板の損傷を避けることができる。As described above, according to the present invention, in an apparatus for processing a substrate to be processed by fixing the substrate to be processed to the electrode by electrostatic adsorption under reduced pressure, the electrostatic adsorption electrode The effect is that the substrate to be processed can be quickly and easily removed from the substrate. In addition, it is possible to avoid damage to the substrate caused by the residual electrostatic attraction force.
【図1】本発明の第1実施例の構成図である。FIG. 1 is a configuration diagram of a first embodiment of the present invention.
【図2】本発明の第2実施例の構成図である。FIG. 2 is a configuration diagram of a second embodiment of the present invention.
【図3】本発明の第3実施例の構成図である。FIG. 3 is a configuration diagram of a third embodiment of the present invention.
【図4】機械的離脱力付与手段を構成したピンの配置関
係を示す上面図である。FIG. 4 is a top view showing an arrangement relationship of pins that constitute a mechanical separating force applying unit.
【図5】機械的離脱力付与手段の別の実施例の一部断面
図である。FIG. 5 is a partial cross-sectional view of another embodiment of the mechanical releasing force applying means.
1 ガスパイプ 2 静電吸着電極 3 誘電体シート 4 直流電源 5 被処理基板 6 電極保持体 7 自動圧力制御機構 7a 流量制御弁 7b 排気系 8 プラズマ源 9 リフトピン 10 真空槽 11a、11b 軸受 12 フレーム 13 駆動軸 13a 駆動部材 14 高周波電源 15 接地電極 20 エッチングガス供給源 21 雰囲気ガス供給源 22 駆動機構 23 シーケンサ 24 円形台 1 Gas Pipe 2 Electrostatic Adsorption Electrode 3 Dielectric Sheet 4 DC Power Supply 5 Substrate 6 Electrode Holder 7 Automatic Pressure Control Mechanism 7a Flow Control Valve 7b Exhaust System 8 Plasma Source 9 Lift Pin 10 Vacuum Tank 11a, 11b Bearing 12 Frame 13 Drive Axis 13a Drive member 14 High frequency power supply 15 Ground electrode 20 Etching gas supply source 21 Atmosphere gas supply source 22 Drive mechanism 23 Sequencer 24 Circular platform
───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.6 識別記号 庁内整理番号 FI 技術表示箇所 H01L 21/3065 // H05H 1/46 M 9014−2G ─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 6 Identification code Office reference number FI technical display location H01L 21/3065 // H05H 1/46 M 9014-2G
Claims (24)
き、前記電極と被処理基板との間の直流電位差による静
電吸着によって被処理基板の固定を行なう静電吸着クラ
ンプ機構を備え、減圧下で被処理基板の加工処理を行な
うプラズマ処理装置において、被処理基板の離脱動作が
行なわれるチャンバーに、静電吸着電極面から突出可能
なピンもしくはピストン等の機械的離脱力付与手段と、
空気、希ガス、無機ガスもしくは窒素、酸素、水素、イ
オウ、塩素またはフッ素原子のうち少なくとも1種を含
む混合ガスを被処理基板周辺に供給する為のガス導入機
構とを備えると共に、被処理基板の離脱動作が行なわれ
るチャンバー内の圧力を所定の圧力に保持するための圧
力制御系を備えたことを特徴とするプラズマ処理装置。1. An electrostatic attraction clamp mechanism for placing a substrate to be processed on an electrode via a dielectric and fixing the substrate to be processed by electrostatic attraction due to a DC potential difference between the electrode and the substrate to be processed. In a plasma processing apparatus for processing a substrate to be processed under reduced pressure, a chamber for performing the operation of separating the substrate to be processed is provided with a mechanical separating force applying means such as a pin or a piston capable of projecting from the electrostatic attraction electrode surface. ,
The substrate to be processed is provided with a gas introduction mechanism for supplying air, a rare gas, an inorganic gas or a mixed gas containing at least one of nitrogen, oxygen, hydrogen, sulfur, chlorine or fluorine atoms to the periphery of the substrate to be processed. A plasma processing apparatus comprising a pressure control system for maintaining the pressure in the chamber in which the detachment operation is performed at a predetermined pressure.
よび圧力制御系に対するシーケンサを更に備えている請
求項1記載のプラズマ処理装置。2. The plasma processing apparatus according to claim 1, further comprising a sequencer for the mechanical release force applying means, the gas introduction mechanism, and the pressure control system.
板との間に印加した直流電圧又は、電極と、被処理基板
の置かれた真空槽内に発生させたプラズマによる被処理
基板の自己バイアスにより生じる電位差で静電吸着させ
て固定を行なうことを特徴とする請求項1または2記載
のプラズマ処理装置。3. Fixing by electrostatic attraction is performed by applying a DC voltage applied between an electrode and a substrate to be processed or a substrate to be processed by plasma generated in a vacuum chamber in which the electrode and the substrate to be processed are placed. The plasma processing apparatus according to claim 1, wherein the plasma processing apparatus is electrostatically attracted and fixed by a potential difference generated by self-bias.
理を行なうプラズマ処理のプロセスガスの導入機構と共
通又は別個とした請求項1または2記載のプラズマ処理
装置。4. The plasma processing apparatus according to claim 1, wherein the gas introduction mechanism is common or separate from the process gas introduction mechanism of the plasma processing for processing the substrate to be processed.
の吸着面内の、被処理基板の縁部以外の位置に設けてあ
る請求項1または2記載のプラズマ処理装置。5. The plasma processing apparatus according to claim 1, wherein the mechanical separating force applying means is provided at a position other than the edge portion of the substrate to be processed within the attraction surface of the electrostatic attraction electrode.
の吸着面内の円周に沿って、等間隔で突没自在に設けた
複数のピンで構成した請求項1または2記載のプラズマ
処理装置。6. The mechanical releasing force applying means comprises a plurality of pins provided so as to project and retract at equal intervals along the circumference of the attraction surface of the electrostatic attraction electrode. Plasma processing equipment.
の吸着面内に、吸着面と面一で、突没自在に設けた円形
台で構成した請求項1または2記載のプラズマ処理装
置。7. The plasma processing according to claim 1 or 2, wherein the mechanical separating force applying means is constituted by a circular base provided in the attraction surface of the electrostatic attraction electrode so as to be flush with the attraction surface so as to be retractable. apparatus.
形台の吸着面から突出する高さを調節する駆動機構を有
する請求項6または7記載のプラズマ処理装置。8. The plasma processing apparatus according to claim 6, wherein the mechanical separating force applying means has a drive mechanism for adjusting a height of the pin or the circular base protruding from the suction surface.
た被処理基板を離脱する方法であって、前記被処理基板
に静電吸着電極の吸着面から突出可能なピンもしくはピ
ストン等の機械的離脱力付与手段を用いて離脱力を与え
ると共に、被処理基板の近傍において、空気、希ガス、
無機ガスもしくは窒素、酸素、水素、イオウ、塩素また
はフッ素原子のうち少なくとも1種を含むガスの所定圧
力雰囲気を維持することを特徴とする被処理基板の離脱
方法。9. A method of releasing a substrate to be processed fixed to an electrostatic attraction electrode by electrostatic attraction, comprising a machine such as a pin or a piston capable of protruding from the attraction surface of the electrostatic attraction electrode to the substrate to be processed. The release force is applied by using the selective release force application means, and in the vicinity of the substrate to be processed, air, rare gas,
A method for separating a substrate to be processed, characterized in that a predetermined pressure atmosphere of an inorganic gas or a gas containing at least one of nitrogen, oxygen, hydrogen, sulfur, chlorine or fluorine atoms is maintained.
基板を離脱する方法であって、前記被処理基板と静電吸
着電極の吸着面の間に微間隙を形成することによって、
被処理基板の近傍で放電を発生させた後、被処理基板を
静電吸着電極から引き離すことを特徴とする被処理基板
の離脱方法。10. A method of separating a substrate to be processed electrostatically attracted to an electrostatic attraction electrode, comprising forming a fine gap between the substrate to be processed and the attraction surface of the electrostatic attraction electrode,
A method for separating a substrate to be processed, comprising: discharging a substrate in the vicinity of the substrate to be processed, and then separating the substrate from the electrostatic attraction electrode.
に存在するガスの圧力を所定圧力に設定した後に行う請
求項10記載の被処理基板の離脱方法。11. The method for separating a substrate to be processed according to claim 10, wherein the fine gap is formed after the pressure of the gas existing in the atmosphere around the substrate is set to a predetermined pressure.
の雰囲気中に存在するガスの圧力を所定圧力に設定する
請求項10記載の被処理基板の離脱方法。12. The method for separating a substrate to be processed according to claim 10, wherein the pressure of the gas existing in the atmosphere around the substrate to be processed is set to a predetermined pressure after forming the fine gap.
間隙は、約0.1mmから約1mmの微間隙とする請求項1
0乃至12のいずれか1項記載の被処理基板の離脱方
法。13. The fine gap formed between the substrate to be processed and the suction surface is a fine gap of about 0.1 mm to about 1 mm.
13. The method for separating a substrate to be processed according to any one of 0 to 12.
ガスの圧力は、0.1Paから500Paの圧力にする
請求項9乃至13のいずれか1項記載の被処理基板の離
脱方法。14. The method for separating a substrate to be processed according to claim 9, wherein the pressure of the gas existing in the atmosphere around the substrate to be processed is set to a pressure of 0.1 Pa to 500 Pa.
せる放電は、DC放電とした請求項9乃至14のいずれ
か1項記載の被処理基板の離脱方法。15. The method for separating a substrate to be processed according to claim 9, wherein the discharge generated between the substrate to be processed and the electrostatic attraction electrode is a DC discharge.
離しは、被処理基板と静電吸着電極との電位差が、放電
を維持するのに必要とする電位以下になったときに行う
請求項9乃至15のいずれか1項記載の被処理基板の離
脱方法。16. The separation of the substrate to be processed from the electrostatic attraction electrode is performed when the potential difference between the substrate to be processed and the electrostatic attraction electrode becomes equal to or lower than a potential required to maintain discharge. 16. The method for separating a substrate to be processed according to any one of 9 to 15.
が220V以下となったときに、被処理基板の静電吸着
電極からの引き離しを行う請求項16記載の被処理基板
の離脱方法。17. The method for detaching a substrate to be processed according to claim 16, wherein the substrate to be processed is separated from the electrostatic attraction electrode when the surface potential of the substrate to be processed having a diameter of 8 inches becomes 220 V or less.
スを流量200sccmで導入し、圧力を20Paに設
定する請求項9乃至17のいずれか1項記載の被処理基
板の離脱方法。18. The method for separating a substrate to be processed according to claim 9, wherein nitrogen gas is introduced into the atmosphere around the substrate to be processed at a flow rate of 200 sccm and the pressure is set to 20 Pa.
ガスは、被処理基板離脱前に被処理基板を処理するガス
とする請求項9乃至17のいずれか1項記載の被処理基
板の離脱方法。19. The separation of the substrate to be processed according to claim 9, wherein the gas existing in the atmosphere around the substrate to be processed is a gas for processing the substrate to be processed before the separation of the substrate to be processed. Method.
ガスとO2 ガスの混合ガスとする請求項19記載の被処
理基板の離脱方法。20. A gas for processing a substrate to be processed is CF 4
The method for separating a substrate to be processed according to claim 19, wherein the mixed gas of gas and O 2 gas is used.
ガスとCHF3 ガスの混合ガスとする請求項19記載の
被処理基板の離脱方法。21. The gas for processing the substrate to be processed is CF 4
The method for separating a substrate to be processed according to claim 19, wherein the mixed gas of gas and CHF 3 gas is used.
けてピン又は円形台を突出させて行う請求項10乃至1
2のいずれか1項記載の被処理基板の離脱方法。22. The fine gap is formed by projecting a pin or a circular base from the suction surface toward the substrate.
3. The method for separating a substrate to be processed according to any one of 2 above.
基板が破損しない程度の高さとする請求項22記載の被
処理基板の離脱方法。23. The method for separating a substrate to be processed according to claim 22, wherein the projecting height of the pin or the circular base is such a height that the substrate is not damaged.
1mmから約1mmの高さとする請求項23記載の被処理基
板の離脱方法。24. The protruding height of the pin or the circular base is about 0.
The method for separating a substrate to be processed according to claim 23, wherein the height is from 1 mm to about 1 mm.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP424095A JP3671379B2 (en) | 1994-02-03 | 1995-01-13 | Plasma processing apparatus having mechanism for removing electrostatically attracted substrate and method for removing electrostatically attracted substrate |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6-11798 | 1994-02-03 | ||
| JP1179894 | 1994-02-03 | ||
| JP424095A JP3671379B2 (en) | 1994-02-03 | 1995-01-13 | Plasma processing apparatus having mechanism for removing electrostatically attracted substrate and method for removing electrostatically attracted substrate |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH07263531A true JPH07263531A (en) | 1995-10-13 |
| JP3671379B2 JP3671379B2 (en) | 2005-07-13 |
Family
ID=26337978
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|---|---|---|---|
| JP424095A Expired - Lifetime JP3671379B2 (en) | 1994-02-03 | 1995-01-13 | Plasma processing apparatus having mechanism for removing electrostatically attracted substrate and method for removing electrostatically attracted substrate |
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Cited By (18)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH1116994A (en) * | 1997-06-20 | 1999-01-22 | Hitachi Ltd | How to remove a sample that has been electrostatically attracted |
| EP0798775A3 (en) * | 1996-03-26 | 1999-07-07 | Nec Corporation | Semiconductor wafer chucking device and method for removing semiconductor wafer |
| KR20020008780A (en) * | 2000-07-20 | 2002-01-31 | 조셉 제이. 스위니 | Method and apparatus for dechucking a substrate |
| KR20030019254A (en) * | 2001-08-30 | 2003-03-06 | 닛본 덴기 가부시끼가이샤 | Wafer holder protecting wafer against electrostatic breakdown |
| JP2005183959A (en) * | 2003-12-15 | 2005-07-07 | Asml Netherlands Bv | Lithographic apparatus and device manufacturing method |
| US7349060B2 (en) | 2003-12-02 | 2008-03-25 | Lg.Philips Lcd Co., Ltd. | Loader and bonding apparatus for fabricating liquid crystal display device and loading method thereof |
| JP2008112139A (en) * | 2006-10-30 | 2008-05-15 | Applied Materials Inc | Mask etching plasma reactor with backside optical sensor and multi-frequency control of etching distribution |
| KR101141025B1 (en) * | 2006-02-07 | 2012-05-04 | 주성엔지니어링(주) | Lift pin drive device |
| JP2012212709A (en) * | 2011-03-30 | 2012-11-01 | Tokyo Electron Ltd | Substrate removing method and storage medium |
| JP2012212710A (en) * | 2011-03-30 | 2012-11-01 | Tokyo Electron Ltd | Substrate removing method and storage medium |
| JP2013149935A (en) * | 2011-12-20 | 2013-08-01 | Tokyo Electron Ltd | Withdrawal control method and plasma processing device |
| JP2014056928A (en) * | 2012-09-12 | 2014-03-27 | Tokyo Electron Ltd | Releasing control method, and plasma processing apparatus |
| KR20200120588A (en) * | 2011-10-05 | 2020-10-21 | 어플라이드 머티어리얼스, 인코포레이티드 | Symmetric plasma process chamber |
| CN111863691A (en) * | 2019-04-26 | 2020-10-30 | 东京毅力科创株式会社 | Electricity elimination method and substrate processing device |
| CN112763812A (en) * | 2020-12-30 | 2021-05-07 | 西安理工大学 | Electrostatic scanning measurement system based on optical interference principle |
| CN115881610A (en) * | 2022-12-07 | 2023-03-31 | 锐立平芯微电子(广州)有限责任公司 | A method and device for controlling the movement speed of a jacking mechanism |
| JPWO2023100452A1 (en) * | 2021-12-03 | 2023-06-08 | ||
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-
1995
- 1995-01-13 JP JP424095A patent/JP3671379B2/en not_active Expired - Lifetime
Cited By (23)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0798775A3 (en) * | 1996-03-26 | 1999-07-07 | Nec Corporation | Semiconductor wafer chucking device and method for removing semiconductor wafer |
| JPH1116994A (en) * | 1997-06-20 | 1999-01-22 | Hitachi Ltd | How to remove a sample that has been electrostatically attracted |
| KR20020008780A (en) * | 2000-07-20 | 2002-01-31 | 조셉 제이. 스위니 | Method and apparatus for dechucking a substrate |
| KR20030019254A (en) * | 2001-08-30 | 2003-03-06 | 닛본 덴기 가부시끼가이샤 | Wafer holder protecting wafer against electrostatic breakdown |
| US7349060B2 (en) | 2003-12-02 | 2008-03-25 | Lg.Philips Lcd Co., Ltd. | Loader and bonding apparatus for fabricating liquid crystal display device and loading method thereof |
| JP2005183959A (en) * | 2003-12-15 | 2005-07-07 | Asml Netherlands Bv | Lithographic apparatus and device manufacturing method |
| KR101141025B1 (en) * | 2006-02-07 | 2012-05-04 | 주성엔지니어링(주) | Lift pin drive device |
| JP2008112139A (en) * | 2006-10-30 | 2008-05-15 | Applied Materials Inc | Mask etching plasma reactor with backside optical sensor and multi-frequency control of etching distribution |
| JP2012212709A (en) * | 2011-03-30 | 2012-11-01 | Tokyo Electron Ltd | Substrate removing method and storage medium |
| JP2012212710A (en) * | 2011-03-30 | 2012-11-01 | Tokyo Electron Ltd | Substrate removing method and storage medium |
| KR20200120588A (en) * | 2011-10-05 | 2020-10-21 | 어플라이드 머티어리얼스, 인코포레이티드 | Symmetric plasma process chamber |
| US11315760B2 (en) | 2011-10-05 | 2022-04-26 | Applied Materials, Inc. | Symmetric plasma process chamber |
| JP2013149935A (en) * | 2011-12-20 | 2013-08-01 | Tokyo Electron Ltd | Withdrawal control method and plasma processing device |
| US9966291B2 (en) | 2012-09-12 | 2018-05-08 | Tokyo Electron Limited | De-chuck control method and plasma processing apparatus |
| KR20150053899A (en) * | 2012-09-12 | 2015-05-19 | 도쿄엘렉트론가부시키가이샤 | Detachment control method and plasma processing device |
| JP2014056928A (en) * | 2012-09-12 | 2014-03-27 | Tokyo Electron Ltd | Releasing control method, and plasma processing apparatus |
| CN111863691A (en) * | 2019-04-26 | 2020-10-30 | 东京毅力科创株式会社 | Electricity elimination method and substrate processing device |
| CN112763812A (en) * | 2020-12-30 | 2021-05-07 | 西安理工大学 | Electrostatic scanning measurement system based on optical interference principle |
| CN112763812B (en) * | 2020-12-30 | 2022-10-14 | 西安理工大学 | An Electrostatic Scanning Measurement System Based on Optical Interference Principle |
| JPWO2023100452A1 (en) * | 2021-12-03 | 2023-06-08 | ||
| WO2023100452A1 (en) * | 2021-12-03 | 2023-06-08 | 株式会社アルバック | Vacuum processing device |
| CN115881610A (en) * | 2022-12-07 | 2023-03-31 | 锐立平芯微电子(广州)有限责任公司 | A method and device for controlling the movement speed of a jacking mechanism |
| KR102868769B1 (en) * | 2025-04-07 | 2025-10-16 | 주식회사 테스 | Substrate processing apparatus |
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