JPH0422152A - Electrostatic attraction equipment - Google Patents

Electrostatic attraction equipment

Info

Publication number
JPH0422152A
JPH0422152A JP2127581A JP12758190A JPH0422152A JP H0422152 A JPH0422152 A JP H0422152A JP 2127581 A JP2127581 A JP 2127581A JP 12758190 A JP12758190 A JP 12758190A JP H0422152 A JPH0422152 A JP H0422152A
Authority
JP
Japan
Prior art keywords
voltage
wafer
electrode
electrostatic
terminals
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP2127581A
Other languages
Japanese (ja)
Other versions
JP2824928B2 (en
Inventor
Masaki Kondo
昌樹 近藤
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Tokyo Electron Ltd
Original Assignee
Tokyo Electron Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Tokyo Electron Ltd filed Critical Tokyo Electron Ltd
Priority to JP12758190A priority Critical patent/JP2824928B2/en
Priority to US07/687,552 priority patent/US5179498A/en
Publication of JPH0422152A publication Critical patent/JPH0422152A/en
Application granted granted Critical
Publication of JP2824928B2 publication Critical patent/JP2824928B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Container, Conveyance, Adherence, Positioning, Of Wafer (AREA)

Abstract

PURPOSE:To increase attractive force by eliminating the period when an AC voltage applied to an electrode becomes zero. CONSTITUTION:A dielectric member 22 composed of polyimide or the like is arranged on a base stand 21. Three electrode layers 23A-23C having the respective fan shapes of 120 deg. angle interval are buried in the dielectric member 22. Terminals 24A-24C are led out from the electrode layer 23A-23C, respectively. Series circuits of power supplies 25UV, W and switches 26UV, W are connected between the terminals 24A and 24B of all retaining parts 2 on a disk 1, respectively. Hence it does not happen that the instantaneous value becomes zero as in the case of single phase AC voltage, and sufficiently intensive electrostatic attractive force can be obtained.

Description

【発明の詳細な説明】[Detailed description of the invention] 【産業上の利用分野】[Industrial application field]

この発明は静電吸着装置に関する。 The present invention relates to an electrostatic chuck device.

【従来の技術】[Conventional technology]

例えば、半導体製造装置のうちのイオン注入装置やスパ
ッタ装置の真空処理装置等においては、被処理体として
のウェーハを真空中で保持搬送して処理する必要かある
ため、その吸着保持手段としては、大気中における吸着
保持手段として広く使用されている真空吸着手段を使用
することかできない。このため、例えばイオン注入装置
では、保持爪によりウェーハの周囲を保持するようにし
ているが、ウェーハと爪との接触によりパーティクル発
生の問題かあった。 そこで、真空中における吸着保持手段として静電吸着装
置か提案されている(特開昭59−79545号公報、
特公平1−36707号公報等)。 これらの静電吸着装置のうちの1つは、吸着保持台のウ
ェーハの吸着面が誘電体で構成され、この誘電体の下部
に、あるいはこの誘電体内に吸着面とほぼ等しい面積に
わたって導電電極層を設け、この電極層とウェーハとの
間に直流電圧を印加する方式である。この方式は、直流
電圧印加により誘電体を介して蓄積される電極層の電荷
と、この電荷とは異種のウェーハの電荷間に静電吸引力
(クーロン力)か発生し、ウェーハか吸着保持台に吸引
されて保持されるである。この方式の場合、ウェーハに
電極を接触させるため、やはりバーティクルの発生の問
題かある。 前記光に提案されている静電吸着装置の他の方式は保持
台の前記吸着面に第1及び第2の吸着部を設け、これら
第1及び第2の吸着部の電極層間に直流電圧を印加する
方式である。この方式は、ウェーハは導電体であるから
静電誘導によって吸着保持台側とは異種の電荷かウェー
ハに現れ、この電荷と電極層への電圧印加により生じた
電荷との間で静電吸引力を生じるものである。この方式
によれば、ウェーハに電極を接触させることはないから
、パーティクルの発生は少なくなる。なお、前記公報に
は、前記電極層とウェーハ間、あるいは第1及び第2の
吸着部の電極間に単相交流を印加する方式も記載されて
いる。
For example, in the vacuum processing equipment of ion implantation equipment and sputtering equipment in semiconductor manufacturing equipment, it is necessary to hold and transport the wafer as the object to be processed in a vacuum, so the suction and holding means is It is only possible to use vacuum adsorption means, which is widely used as an adsorption/holding means in the atmosphere. For this reason, for example, in an ion implantation apparatus, the periphery of the wafer is held by a holding claw, but there is a problem in that particles are generated due to contact between the wafer and the claw. Therefore, an electrostatic adsorption device has been proposed as an adsorption/holding means in vacuum (Japanese Unexamined Patent Publication No. 79545/1983,
(Special Publication No. 1-36707, etc.). In one of these electrostatic adsorption devices, the wafer adsorption surface of the adsorption/holding table is composed of a dielectric material, and a conductive electrode layer is provided below or within this dielectric material over an area approximately equal to the adsorption surface. In this method, a DC voltage is applied between the electrode layer and the wafer. In this method, an electrostatic attraction force (Coulomb force) is generated between the charge on the electrode layer accumulated through the dielectric material by applying a DC voltage and the charge on the wafer, which is different from this charge. It is attracted to and held. In this method, since the electrode is brought into contact with the wafer, there is still the problem of verticle generation. Another method of the electrostatic adsorption device proposed for the light is to provide first and second adsorption parts on the adsorption surface of the holding table, and apply a DC voltage between the electrode layers of these first and second adsorption parts. This is a method of applying voltage. In this method, since the wafer is a conductor, a different type of charge appears on the wafer due to electrostatic induction, and an electrostatic attraction force is generated between this charge and the charge generated by applying voltage to the electrode layer. It is something that causes According to this method, the generation of particles is reduced because the electrode is not brought into contact with the wafer. Note that the publication also describes a method of applying single-phase alternating current between the electrode layer and the wafer or between the electrodes of the first and second suction parts.

【発明が解決しようとする課題】[Problem to be solved by the invention]

ところで、直流電圧をウェーハと電極間または2電極間
に印加する方式の場合、吸引力(クーロン力)は、強力
であるか、吸着面の誘電体に誘電分極か生じるため、電
圧印加を停止しても電荷か残留し、このため被吸着物か
吸着保持台から離脱しにくいという欠点かある。また、
被吸着物にコミなどが付着しやすいという欠点もある。 一方、直流電圧の代わりに交流電圧を印加すれば、ゴミ
か被吸着物に付着するのを少なくてきると共に、前記誘
電体には誘電分極か生しないため、電圧印加を停止すれ
ば被吸着物は即座に吸着保持台から離脱できる。ところ
が、前述の公報記載の従来技術の場合、印加されるのは
単相交流電圧であるため、十分な吸引力を得ることがで
きない。 すなわち、単相交流電圧は、印加瞬時電圧か一定周期で
必ず零ボルトになり、その瞬時電圧時点ては吸引力も零
になってしまうからである。 この発明は、以上の点に鑑み、印加する電圧として交流
電圧を用いることができ、しかも吸引力の大きい静電吸
着装置を提供することを目的とする。
By the way, in the case of a method in which DC voltage is applied between the wafer and the electrode or between two electrodes, the attractive force (Coulomb force) is strong or dielectric polarization occurs in the dielectric material on the attracting surface, so the voltage application must be stopped. However, there is a disadvantage that some charge remains, which makes it difficult for the object to be attracted to separate from the suction and holding table. Also,
Another drawback is that dust and the like tend to adhere to the object to be absorbed. On the other hand, if an alternating current voltage is applied instead of a direct current voltage, the amount of dust or dirt adhering to the object to be attracted will be reduced, and since dielectric polarization will not occur in the dielectric material, if the voltage application is stopped, the object to be attracted will be can be immediately removed from the suction holding table. However, in the case of the prior art described in the above-mentioned publication, since a single-phase AC voltage is applied, a sufficient attraction force cannot be obtained. That is, the instantaneous voltage applied to the single-phase AC voltage always becomes zero volts at a certain period, and the attractive force also becomes zero at the moment of the instantaneous voltage. In view of the above points, it is an object of the present invention to provide an electrostatic adsorption device that can use an alternating current voltage as the applied voltage and has a large attraction force.

【課題を解決するための手段】[Means to solve the problem]

この発明は、被吸着体と接触すべき面が誘電体で構成さ
れると共に、この誘電体の下方または誘電体内に電極か
設けられ、この電極に交流電圧を印加して、前記被吸着
体を静電吸引力により吸着する静電吸着装置において、 前記電極に印加する交流電圧か零電圧になる期間を無く
すようにしたことを特徴とする。
In this invention, the surface to be in contact with the object to be attracted is made of a dielectric material, and an electrode is provided below or within the dielectric, and an alternating current voltage is applied to this electrode to attract the object to be attracted. An electrostatic adsorption device that adsorbs by electrostatic attraction force is characterized in that a period in which the AC voltage applied to the electrode becomes zero voltage is eliminated.

【作用】[Effect]

この発明は、静電吸着用の3個以上の電極間に、位相か
すれた3相以上の交流電圧を印加するので、吸着印加電
圧の瞬時値か零になることはなく、比較的大きい静電吸
引力か得られる。
In this invention, an AC voltage of three or more phases with a blurred phase is applied between three or more electrodes for electrostatic adsorption, so that the instantaneous value of the applied adsorption voltage does not become zero, and relatively large electrostatic You can get some suction power.

【実施例】【Example】

以下、この発明による静電吸着装置を高電流タイプのイ
オン注入装置に適用した場合の一実施例を、図を参照し
ながら説明する。 第4図に示すように、高電流タイプのイオン注入装置は
、イオンを注入することによる発熱を緩和する目的から
、真空室内に配されるディスク1上に、その円周方向に
沿って複数の半導体ウェーハの保持部2を設け、この保
持部2に半導体つ工−ハ3を保持させ、ディスク1をそ
の中心位置を回転軸として、例えば矢印4て示す方向に
回転させると共に、ディスク1を例えば矢印5で示す方
向に往復直線運動させ、複数個の半導体ウェーハ3に対
して、−括してイオンを注入する構成か採られている。 各保持部2は、静電吸着機構を有するもので、第2図の
断面図に示すように、例えばシリコンコムからなる基台
21の上に、例えばポリイミド等のプラスチックからな
る誘電体22か設けられる。 この誘電体22内には、ウェーハ吸着期間、吸着印加電
圧か零になる瞬時期間を無くす手段として、例えば第1
図に示すように、この例ではそれぞれ120°の旬間隔
分の扇形の形状の3個の電極層23A、23B、23C
か埋め込まれて、サンドイッチ状の構造を有している。 この例の場合、誘電体22の厚さは、電極層を含めて、
例えば25廓程度とされている。 そして、各電極層23A、23B、23Cからは、端子
24A、24B、24Cが導出される。 そして、ディスク1上のすへての保持部2の、端子24
A及び24B間には第3図Aに示す交流電圧Elを発生
する電源25Uとスイッチ260との直列回路か接続さ
れ、端子24B及び24C間には第3図Bに示す交流電
圧EV(交流電圧EUとは]20°位相か異なる)を発
生する電源25Vとスイッチ26Vとの直列回路が接続
され、端子24C及び24A間には第3図Cに示す交流
電圧EW(交流電圧EUとは2406位相が異なる)を
発生する電源25Wとスイッチ26Wとの直列回路か接
続される。電源25U、25V、25Wとしては、商用
の3相交流電源を用いるこ、とができる。 この場合、スイッチ26U、26V、26Wは、互いに
連動するようにされ、ウェーハ3が保持部2に載置され
たとき、オンとされる。スイッチ26U、26V、26
Wかオンとされると、各電極層23A、23B、23C
間に前記交流電圧EUEV、EWが印加される。すると
、誘電体22を介して静電誘導により導電体であるウェ
ーハ3に電荷が現れ、クーロン力により保持部2に吸着
される。 この場合、電極層23A、23B、23Cに印加される
電圧は、第3図に示したように、3相交流電圧であるの
で、単相交流電圧のように瞬時値か零になることはなく
、十分な強さの静電吸引力か得られる。 なお、保持部2の基台21はアルミニウムやセラミック
で構成することもてきる。しかし、上記の例にように、
基台21をシリコンゴム等の弾性材料で構成した場合に
は、ウェーハ3に反り等があったとき、誘電体22は極
く薄いフレキシブル基板と同様の構成であるから、その
ウェーハの反りの形状に応じて基台21が変形する。し
たがって、ウェーハ3に反り等の変形があっても保持部
2との間に隙間が生じることはなく、所定値以上の強さ
の吸引力を保持することができる。 なお、電極数及び位相のずれた交流電圧の数は、3以上
であっても勿論良い。 また、上記実施例では、ウェーハの静電吸着電圧印加領
域を3領域にした例について説明したが、−電極で多相
交流電圧を印加しても、印加される吸着電圧かウェーハ
に対して零期間を無いようにすればよい。さらに、直流
バイアスを持たせてもよい。この場合の直流バイアス電
圧は、低電圧のの方かよい。 また、以上の例は、イオン注入装置にこの発明による静
電吸着装置を適用した場合であるが、冒頭でも述べたよ
うに、この発明は、スパッタ装置、その他の真空処理装
置及び真空的搬送装置にも適用できることはいうまでも
ない。 また、真空内に限らず、大気中における被吸着体の保持
、搬送にも適用可能である。 さらに、被吸着体としては、半導体ウェーハに限らず、
導電性のものであれば適用可能である。
An embodiment in which the electrostatic adsorption device according to the present invention is applied to a high current type ion implantation device will be described below with reference to the drawings. As shown in FIG. 4, a high-current type ion implanter has a plurality of ion implanters installed on a disk 1 placed in a vacuum chamber along its circumferential direction in order to alleviate heat generation caused by ion implantation. A semiconductor wafer holding part 2 is provided, the semiconductor wafer 3 is held in the holding part 2, and the disk 1 is rotated, for example, in the direction shown by the arrow 4, with the center position as the rotation axis, and the disk 1 is, for example, A configuration is adopted in which ions are implanted into a plurality of semiconductor wafers 3 at once by making a reciprocating linear movement in the direction shown by the arrow 5. Each holding part 2 has an electrostatic adsorption mechanism, and as shown in the cross-sectional view of FIG. It will be done. In this dielectric body 22, for example, a first
As shown in the figure, in this example, three fan-shaped electrode layers 23A, 23B, and 23C each have an interval of 120°.
It has a sandwich-like structure. In this example, the thickness of the dielectric 22, including the electrode layer, is
For example, it is said to be about 25 ku. Terminals 24A, 24B, and 24C are led out from each electrode layer 23A, 23B, and 23C. Then, the terminal 24 of the entire holding part 2 on the disk 1
A and 24B are connected between a series circuit of a power supply 25U and a switch 260 that generate an AC voltage El shown in FIG. 3A, and between terminals 24B and 24C are connected an AC voltage EV (AC voltage A series circuit of a 25V power supply and a 26V switch is connected between terminals 24C and 24A, which generates an AC voltage EW (20° phase difference between EU and EU) as shown in Figure 3C. A series circuit of a power supply 25W and a switch 26W, which generates a power of 25W and 26W, is connected. As the power source 25U, 25V, and 25W, a commercial three-phase AC power source can be used. In this case, the switches 26U, 26V, and 26W are made to interlock with each other, and are turned on when the wafer 3 is placed on the holding section 2. Switch 26U, 26V, 26
When W is turned on, each electrode layer 23A, 23B, 23C
The alternating current voltages EUEV and EW are applied between them. Then, charges appear on the wafer 3, which is a conductor, through the dielectric 22 due to electrostatic induction, and are attracted to the holding portion 2 by Coulomb force. In this case, the voltage applied to the electrode layers 23A, 23B, and 23C is a three-phase AC voltage, as shown in FIG. 3, so it does not become an instantaneous value or zero unlike a single-phase AC voltage. , a sufficiently strong electrostatic attraction force can be obtained. Note that the base 21 of the holding portion 2 may be made of aluminum or ceramic. However, as in the example above,
When the base 21 is made of an elastic material such as silicone rubber, when the wafer 3 is warped, the dielectric 22 has the same structure as an extremely thin flexible substrate, so the shape of the warp of the wafer will be corrected. The base 21 deforms accordingly. Therefore, even if the wafer 3 is deformed such as warping, no gap will be created between the wafer 3 and the holding part 2, and a suction force greater than a predetermined value can be maintained. Note that the number of electrodes and the number of phase-shifted AC voltages may of course be three or more. Further, in the above embodiment, an example was explained in which the electrostatic adsorption voltage application area for the wafer was divided into three areas, but even if a multiphase AC voltage is applied at the - electrode, the applied adsorption voltage is zero with respect to the wafer. The period can be set to zero. Furthermore, a DC bias may be provided. In this case, it is better to use a low DC bias voltage. Further, the above example is a case where the electrostatic adsorption device according to the present invention is applied to an ion implantation device, but as stated at the beginning, the present invention is also applicable to sputtering devices, other vacuum processing devices, and vacuum transfer devices. Needless to say, it can also be applied to Moreover, it is applicable not only to the vacuum but also to the holding and transport of the adsorbed object in the atmosphere. Furthermore, the object to be adsorbed is not limited to semiconductor wafers.
Any conductive material can be used.

【発明の効果】【Effect of the invention】

以上説明したように、この発明によれば、交流電圧を電
極間に印加するものであるので、被吸着物へのごみの付
着か少なくなる。また、印加電圧を断った時には、誘電
体に電荷か残留することはないから、被吸着体の離脱は
容易である。 そして、この発明では、3相以上の多相交流電圧を、複
数の電極間に印加するものであるから、所定の静電吸着
力を確保することかできる。
As explained above, according to the present invention, since an alternating current voltage is applied between the electrodes, the amount of dust attached to the object to be attracted is reduced. Furthermore, when the applied voltage is cut off, no charge remains on the dielectric material, so the object to be attracted can easily be removed. Further, in this invention, since a polyphase AC voltage of three or more phases is applied between a plurality of electrodes, a predetermined electrostatic attraction force can be ensured.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、この発明による静電吸着装置の一実施例の平
面図、第2図は、そのA−A断面図、第3図は、位相の
異なる複数の交流電圧の例を示す図、第4図は、この発
明か適用されるイオン注入装置の要部を説明するための
図である。 2、ウェーハの保持部 3・半導体ウェーハ 21、基台 22;誘電体 23A、23B、23C;電極層 2.4A、24B、24C;端子 25U、25V、25W、3相交流電源EU、EV、E
W、3相交流電圧 代理人 弁理士 佐 藤 正 美 f竹IPv面図 第1図 A−A%面図 第2図
FIG. 1 is a plan view of an embodiment of the electrostatic adsorption device according to the present invention, FIG. 2 is a cross-sectional view taken along line A-A, and FIG. 3 is a diagram showing an example of a plurality of alternating current voltages having different phases. FIG. 4 is a diagram for explaining essential parts of an ion implantation apparatus to which the present invention is applied. 2. Wafer holding part 3 - semiconductor wafer 21, base 22; dielectrics 23A, 23B, 23C; electrode layers 2.4A, 24B, 24C; terminals 25U, 25V, 25W, 3-phase AC power source EU, EV, E
W, 3-phase AC voltage agent Patent attorney Tadashi Sato Bifu Bamboo IPv side view Figure 1 A-A% side view Figure 2

Claims (1)

【特許請求の範囲】  被吸着体と接触すべき面が誘電体で構成されると共に
、この誘電体の下方または誘電体内に電極が設けられ、
この電極に交流電圧を印加して、前記被吸着体を静電吸
引力により吸着する静電吸着装置において、 前記電極に印加する交流電圧が零電圧になる期間を無く
すようにしたことを特徴とする静電吸着装置。
[Claims] The surface to be in contact with the object to be attracted is made of a dielectric material, and an electrode is provided below or within the dielectric material,
An electrostatic adsorption device that applies an alternating current voltage to the electrode and adsorbs the object by electrostatic attraction, characterized in that a period in which the alternating current voltage applied to the electrode becomes zero voltage is eliminated. Electrostatic adsorption device.
JP12758190A 1990-05-17 1990-05-17 Electrostatic suction device Expired - Lifetime JP2824928B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP12758190A JP2824928B2 (en) 1990-05-17 1990-05-17 Electrostatic suction device
US07/687,552 US5179498A (en) 1990-05-17 1991-04-19 Electrostatic chuck device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12758190A JP2824928B2 (en) 1990-05-17 1990-05-17 Electrostatic suction device

Publications (2)

Publication Number Publication Date
JPH0422152A true JPH0422152A (en) 1992-01-27
JP2824928B2 JP2824928B2 (en) 1998-11-18

Family

ID=14963605

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12758190A Expired - Lifetime JP2824928B2 (en) 1990-05-17 1990-05-17 Electrostatic suction device

Country Status (1)

Country Link
JP (1) JP2824928B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003332412A (en) * 2002-03-04 2003-11-21 Hitachi High-Technologies Corp Electrostatic chuck equipment and treatment method of substrate using the equipment
JP2015099839A (en) * 2013-11-19 2015-05-28 東京エレクトロン株式会社 Method of attracting object to be attracted onto placing table, and processing apparatus

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003332412A (en) * 2002-03-04 2003-11-21 Hitachi High-Technologies Corp Electrostatic chuck equipment and treatment method of substrate using the equipment
JP2015099839A (en) * 2013-11-19 2015-05-28 東京エレクトロン株式会社 Method of attracting object to be attracted onto placing table, and processing apparatus
US9953854B2 (en) 2013-11-19 2018-04-24 Tokyo Electron Limited Method of adsorbing target object on mounting table and plasma processing apparatus
US10410902B2 (en) 2013-11-19 2019-09-10 Tokyo Electron Limited Plasma processing apparatus

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