JPH0950898A - Plasma treatment device - Google Patents

Plasma treatment device

Info

Publication number
JPH0950898A
JPH0950898A JP7202017A JP20201795A JPH0950898A JP H0950898 A JPH0950898 A JP H0950898A JP 7202017 A JP7202017 A JP 7202017A JP 20201795 A JP20201795 A JP 20201795A JP H0950898 A JPH0950898 A JP H0950898A
Authority
JP
Japan
Prior art keywords
electromagnetic wave
sample
plasma
processing apparatus
plasma processing
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.)
Pending
Application number
JP7202017A
Other languages
Japanese (ja)
Inventor
健 ▲吉▼岡
Takeshi Yoshioka
Tetsunori Kaji
哲徳 加治
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP7202017A priority Critical patent/JPH0950898A/en
Publication of JPH0950898A publication Critical patent/JPH0950898A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To eliminate in-plane ununiformity of an impedance of a pulse bias circuit by providing a conductor which is parallel to a sample and substantially functions as a ground electrode. SOLUTION: Plasma treatment device is provided with a plasma generating chamber 2 for introducing an electromagnetic wave 1 and a discharge gas, a means for introducing the electromagnetic wave 1 therein, and a dielectric window 46 for partitioning the plasma generating chamber 2 and the electromagnetic wave introduction means. It is also provided with a holder 3 on which a sample to be treated using plasma generated by the electromagnetic wave 1 is mounted and a means 5 for applying pulse voltage on the holder 3 as a bias. It is characterized as a structure that a conductor is provided in parallel to the sample and substantially functions as a ground electrode 4a.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、プラズマ処理装置のバ
イアス印加方法および、それを試料全面にわたって均一
に印加するための手段を備えたプラズマ処理装置に関す
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for applying a bias to a plasma processing apparatus and a plasma processing apparatus equipped with a means for uniformly applying the bias to the entire surface of a sample.

【0002】[0002]

【従来の技術】従来、プラズマおよび、試料に印加する
高周波バイアスを用いて、試料を加工又は推積するドラ
イエッチング又はCVD装置においては、電子シェイデ
ィング効果と呼ぶ試料へのチャージアップ現象ならび
に、それに起因する加工形状の乱れ(主にドライエッチ
ングにおけるノッチング)が問題となっている。そのた
めバイアス高周波として、パルス電源を用い正の短パル
スを加えることによって、電子を試料に引っ込み、正に
チャージアップした試料を電気的に中和し、それによっ
てノッチングを押さえる提案が、たとえば特開平6−6
1182号公報等において行なわれている。
2. Description of the Related Art Conventionally, in a dry etching or CVD apparatus for processing or depositing a sample by using plasma and a high frequency bias applied to the sample, a charge-up phenomenon to the sample called electron shading effect and Distortion of the processed shape (mainly notching in dry etching) resulting from this is a problem. Therefore, as a bias high frequency, a positive short pulse is applied by using a pulse power source to pull electrons into the sample to electrically neutralize the sample positively charged up, thereby suppressing notching. -6
1182, etc.

【0003】[0003]

【発明が解決しようとする課題】上記従来技術は、たと
えばくり返し周波数100KHz,duty比1%以
下、パルス幅100ns程度が必要とされている。この
ことは、このパルス波をフーリエスペクトルで考えると
100KHz〜100MHzの帯域を持つことになり、
パルス波形を歪ませないで試料に均等にパルスを印加す
るには特別な工夫が必要となる。すなわち、この場合と
くに問題となるのは、バイアス回路のうちのプラズマを
介して接地電極に至る経路であって、試料中央部から接
地電極に至る経路インピーダンスと、試料端部から接地
電極に至る経路のインピーダンスが同等かつ、広い帯域
幅を持っていなければ、処理の面内不均一や、それに起
因する試料ダメージを引き起こしてしまう問題があっ
た。
The above-mentioned prior art requires, for example, a repetition frequency of 100 KHz, a duty ratio of 1% or less, and a pulse width of about 100 ns. This means that when this pulse wave is considered in the Fourier spectrum, it has a band of 100 KHz to 100 MHz,
Special techniques are required to apply the pulse evenly to the sample without distorting the pulse waveform. That is, in this case, what is particularly problematic is the path from the center of the sample to the ground electrode through the plasma in the bias circuit, and the path impedance from the center of the sample to the ground electrode and the path from the sample end to the ground electrode. If the impedances are the same and do not have a wide bandwidth, there is a problem that in-plane non-uniformity of processing and sample damage caused by the unevenness occur.

【0004】とくに、磁力線を試料にほぼ垂直に印加
し、マイクロ波によってプラズマを発生するECR方式
のプラズマ処理装置においては、接地電極が処理室の側
壁方向にあることが一般的であり、かつ磁力線を横切っ
て流れようとするバイアス回路のインピーダンスが10
〜100MHz帯域においては、非常に大きくなるた
め、試料へのバイアス印加の面内不均一が非常に大きく
なってくる。
Particularly, in an ECR type plasma processing apparatus in which magnetic lines of force are applied substantially perpendicularly to a sample and plasma is generated by microwaves, the ground electrode is generally located in the side wall direction of the processing chamber, and the lines of magnetic force are also present. The impedance of the bias circuit that tries to flow across the
In the band of up to 100 MHz, the in-plane non-uniformity of bias application to the sample becomes very large because it becomes very large.

【0005】本発明の目的は、パルスバイアス回路のイ
ンピーダンスの面内不均一を解消し、試料処理の均一化
を実現するプラズマ処理装置を提供することにある。
An object of the present invention is to provide a plasma processing apparatus which eliminates in-plane nonuniformity of impedance of a pulse bias circuit and realizes uniform sample processing.

【0006】[0006]

【課題を解決するための手段】上記目的を達成するため
に、電磁波と放電ガスが導入されるプラズマ発生室と、
該プラズマ発生室内に前記電磁波を導入する手段と、前
記プラズマ発生室と前記電磁波導入手段とを仕切る誘電
体窓と、前記電磁波により生成したプラズマを用いて処
理すべき試料を載せるホルダーとホルダーへのバイアス
としてパルス電圧を印加する手段を具備したプラズマ処
理装置において、試料に平行かつ、実質的に接地電極と
して機能する導体を設けたことを特徴とするものであ
る。
In order to achieve the above object, a plasma generating chamber into which an electromagnetic wave and a discharge gas are introduced,
A means for introducing the electromagnetic wave into the plasma generation chamber, a dielectric window for partitioning the plasma generation chamber and the electromagnetic wave introduction means, a holder for mounting a sample to be processed using the plasma generated by the electromagnetic wave, and a holder In a plasma processing apparatus equipped with a means for applying a pulse voltage as a bias, a conductor parallel to the sample and substantially functioning as a ground electrode is provided.

【0007】望ましくは、電磁波として、マイクロ波を
用い試料にほぼ直交するように磁力線を発生する手段を
設けたことを特徴とするものである。
Desirably, a means for generating lines of magnetic force is provided so that a microwave is used as the electromagnetic wave so as to be substantially orthogonal to the sample.

【0008】望ましくは誘電体窓に接して全面にわたっ
てほぼ均一に電磁波を透過させる電極を備え、該電極を
実質的にアース電位にしたことを特徴とするものであ
る。
Desirably, an electrode is provided which is in contact with the dielectric window and allows electromagnetic waves to pass substantially uniformly over the entire surface, and the electrode is substantially set to the ground potential.

【0009】望ましくはマイクロ波導入手段として、同
軸導波管を用いたことを特徴とする。
Preferably, a coaxial waveguide is used as the microwave introducing means.

【0010】望ましくは電磁波として、1〜100MH
z帯域の誘導方式高周波を用いたことと特徴とするもの
である。
Preferably, the electromagnetic wave is 1 to 100 MH
It is characterized by using a high frequency inductive method in the z band.

【0011】[0011]

【作用】図2に、プラズマ中の高周波電流パスを等価回
路で表わしたものを示す。この場合とにくマイクロ波E
CRの場合を例にとって記明している。図2においてR
とCは、プラズマ試料間のシースにおける抵抗と容量、
Lは磁力線Bを線横切ってプラズマ中に電流が流れると
きのインダクタンスである。プラズマ中の電子は、磁力
線を横切っては移動出来ないので、イオンが電気伝導を
担うが、慣性のために電流が流れにくく等価的にインダ
クタンスLとして作用する。磁力線を横切るインピーダ
ンスjωLは、理論計算によって1MHzにて、j10
0Ω程であり、周波数に比例するので100MHzにし
ては、j10kΩにも達する。シースのRや1/jωC
は100Ω以下であるので10MHz以上の高周波で
は、jωLが支配する。試料の中央と端部とでは、イン
ピーダンスに大きな差が出来てしまい不均一が生じるこ
とになる。(すなわち、I1とI2に不均衝が生ずる。)
仮に、試料に平行する形で上部に接地電極を置くことが
出来れば、磁力線に平行な方向のインピーダンスは、も
ともと無視出来る程に小さく、かつ試料の中央と端部で
差がなくなるので不均一が解消される。I3とI4が等し
くなる。このことを具体的に実現する方法について、以
下実施例を説明する。
FIG. 2 shows an equivalent circuit of a high frequency current path in plasma. In this case, the microwave E
The case of CR is described as an example. R in FIG.
And C are the resistance and capacitance in the sheath between the plasma samples,
L is an inductance when a current flows in the plasma across the line of magnetic force B. Since the electrons in the plasma cannot move across the lines of magnetic force, the ions are responsible for electrical conduction, but due to inertia, it is difficult for current to flow and equivalently acts as the inductance L. Impedance jωL that crosses the magnetic field line is calculated as j10 at 1 MHz by theoretical calculation.
Since it is about 0Ω and is proportional to the frequency, it reaches j10 kΩ at 100 MHz. R of sheath and 1 / jωC
Is 100Ω or less, so jωL is dominant at high frequencies of 10 MHz or more. There will be a large difference in impedance between the center and the end of the sample, resulting in non-uniformity. (That is, there is a disparity between I 1 and I 2. )
If the ground electrode could be placed on top of the sample in parallel with the sample, the impedance in the direction parallel to the magnetic field lines would originally be so small that it could be ignored, and there would be no difference between the center and the end of the sample, resulting in non-uniformity. Will be resolved. I 3 and I 4 become equal. An embodiment will be described below as a method for specifically realizing this.

【0012】[0012]

【実施例】図1は本発明の第1の実施例を示す図であ
る。マイクロ波ECR装置に応用した例である。図1に
おいて、マイクロ波1は、円形TE11モードにて導波
されプラズマ室2内に導入される。5はパルス電源であ
り、電極3に印加される。TE11モードの場合は、導
波方向に垂直な面上で、電源ベクトルは一方向に揃って
いるので、それに直交するようにスリットを切った導体
を設置してもマイクロ波は、さまたげることなく通過す
る。図1(b)においては、このようなスリット導体4
aをアース電位とし、マイクロ波導入窓4bのところに
とりつけた。このスリット電極4aは、プラズマに直接
さらされて金属汚染をひき起こすことのないよう、たと
えば薄手のカバー石英4cを設置してもよい。厚さは、
これが高周波回路のインピーダンスとして障害にならな
い程度(例えば3mm以下)とする。
FIG. 1 is a diagram showing a first embodiment of the present invention. This is an example applied to a microwave ECR device. In FIG. 1, the microwave 1 is guided in the circular TE11 mode and introduced into the plasma chamber 2. A pulse power source 5 is applied to the electrode 3. In the TE11 mode, the power supply vector is aligned in one direction on the plane perpendicular to the waveguiding direction, so even if a conductor with a slit cut perpendicular to it is installed, microwaves pass through without interruption. To do. In FIG. 1B, such a slit conductor 4
A was set to the ground potential, and it was attached to the microwave introduction window 4b. The slit electrode 4a may be provided with, for example, a thin cover quartz 4c so as not to be directly exposed to plasma and cause metal contamination. The thickness is
The impedance of the high-frequency circuit is set to such a degree that it does not hinder (eg, 3 mm or less).

【0013】図3は、誘導結合高周波プラズマ装置に応
用した例である。誘導プラズマの場合は、同心円状にコ
イル14が巻かれており、プラズマ中へ入る電界ベクト
ル4hもコイルと同じ方向を向いている。したがって、
スリット電極4aとしては、図3(a)に示したような
放射状とすればよい。
FIG. 3 shows an example of application to an inductively coupled high frequency plasma device. In the case of induction plasma, the coil 14 is wound concentrically, and the electric field vector 4h entering the plasma also faces the same direction as the coil. Therefore,
The slit electrodes 4a may have a radial shape as shown in FIG.

【0014】図4は、マイクロ波ECRの場合である
が、マイクロ波を同軸TEMモードで導入する場合の例
を示してある。このような例においては、マイクロ波は
チャンバ上面外周部から出射させる関係上、上面中央部
に接地電極4aを直接とりつけることが出来る。
FIG. 4 shows the case of the microwave ECR, but shows an example of introducing the microwave in the coaxial TEM mode. In such an example, since the microwave is emitted from the outer peripheral portion of the upper surface of the chamber, the ground electrode 4a can be directly attached to the central portion of the upper surface.

【0015】[0015]

【発明の効果】以上説明した如く本発明によれば、パル
スバイアス印加時の試料処理の均一性を確保することが
出来る。
As described above, according to the present invention, it is possible to ensure the uniformity of sample processing when a pulse bias is applied.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の第1の実施例を示す説明図である。FIG. 1 is an explanatory diagram showing a first embodiment of the present invention.

【図2】本発明の原理を示す説明図である。FIG. 2 is an explanatory diagram showing the principle of the present invention.

【図3】本発明の第2の実施例を示す説明図である。FIG. 3 is an explanatory diagram showing a second embodiment of the present invention.

【図4】本発明の第3の実施例を示す説明図である。FIG. 4 is an explanatory view showing a third embodiment of the present invention.

【符号の説明】[Explanation of symbols]

1…マイクロ波、2…処理室、3…試料台、4…導入
窓、4a…接地電極、4b…誘電体、4c…誘電体、5
…パルスバイアス電源、4h…電界ベクトル。
DESCRIPTION OF SYMBOLS 1 ... Microwave, 2 ... Processing chamber, 3 ... Sample stand, 4 ... Introduction window, 4a ... Ground electrode, 4b ... Dielectric material, 4c ... Dielectric material, 5
... pulse bias power supply, 4h ... electric field vector.

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】電磁波と放電ガスが導入されるプラズマ発
生室と、該プラズマ発生室内に前記電磁波を導入する手
段と、前記プラズマ発生室と前記電磁波導入手段とを仕
切る誘導体窓と、前記電磁波により生成したプラズマを
用いて処理すべき試料を載せるホルダーとホルダーへの
バイアスとしてパルス電圧を印加する手段を具備したプ
ラズマ処理装置において、 前記試料に平行かつ実質的に接地電極として機能する導
体を設けたことを特徴とするプラズマ処理装置。
1. A plasma generating chamber into which an electromagnetic wave and a discharge gas are introduced, a means for introducing the electromagnetic wave into the plasma generating chamber, a dielectric window for partitioning the plasma generating chamber and the electromagnetic wave introducing means, and the electromagnetic wave. In a plasma processing apparatus comprising a holder for mounting a sample to be processed using the generated plasma and a means for applying a pulse voltage as a bias to the holder, a conductor is provided parallel to the sample and substantially functioning as a ground electrode. A plasma processing apparatus characterized by the above.
【請求項2】請求項第1項において、前記電磁波として
マイクロ波を用い試料にほぼ直交するように磁力線を発
生する手段を設けたことを特徴とするプラズマ処理装
置。
2. The plasma processing apparatus according to claim 1, further comprising means for generating a magnetic force line so that a microwave is used as the electromagnetic wave so as to be substantially orthogonal to a sample.
【請求項3】請求項1において、前記電磁波として、1
〜100MHz帯域の誘導方式高周波を用いたことを特
徴とするプラズマ処理装置。
3. The electromagnetic wave according to claim 1, wherein the electromagnetic wave is 1
A plasma processing apparatus characterized by using an induction high frequency in the range of up to 100 MHz.
【請求項4】請求項2において、前記誘電体窓に接して
全面にわたってほぼ均一に電磁波を透過させる電極を備
え、該電極を実質的にアース電圧にしたことを特徴とす
るプラズマ処理装置。
4. A plasma processing apparatus according to claim 2, further comprising an electrode which is in contact with said dielectric window and which transmits an electromagnetic wave substantially uniformly over the entire surface thereof, and which is set to a substantially ground voltage.
【請求項5】請求項2において、前記マイクロ波導入手
段として同軸導波管を用いたことを特徴とするプラズマ
処理装置。
5. The plasma processing apparatus according to claim 2, wherein a coaxial waveguide is used as the microwave introducing means.
JP7202017A 1995-08-08 1995-08-08 Plasma treatment device Pending JPH0950898A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7202017A JPH0950898A (en) 1995-08-08 1995-08-08 Plasma treatment device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7202017A JPH0950898A (en) 1995-08-08 1995-08-08 Plasma treatment device

Publications (1)

Publication Number Publication Date
JPH0950898A true JPH0950898A (en) 1997-02-18

Family

ID=16450551

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7202017A Pending JPH0950898A (en) 1995-08-08 1995-08-08 Plasma treatment device

Country Status (1)

Country Link
JP (1) JPH0950898A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2002065820A1 (en) * 2001-02-12 2002-08-22 Se Plasma Inc. Apparatus for generating low temperature plasma at atmospheric pressure
JP2011040481A (en) * 2009-08-07 2011-02-24 Hitachi High-Technologies Corp Plasma processing apparatus using transmission electrode

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2002065820A1 (en) * 2001-02-12 2002-08-22 Se Plasma Inc. Apparatus for generating low temperature plasma at atmospheric pressure
JP2011040481A (en) * 2009-08-07 2011-02-24 Hitachi High-Technologies Corp Plasma processing apparatus using transmission electrode

Similar Documents

Publication Publication Date Title
JP4852189B2 (en) Plasma processing apparatus and plasma processing method
JP3375646B2 (en) Plasma processing equipment
US6172321B1 (en) Method and apparatus for plasma processing apparatus
KR100652983B1 (en) Plasma processing apparatus and method
KR100642157B1 (en) Plasma processing system and method and electrode plate of plasma processing system
JP3290777B2 (en) Inductively coupled high frequency discharge method and inductively coupled high frequency discharge device
JP3482904B2 (en) Plasma processing method and apparatus
US5432315A (en) Plasma process apparatus including ground electrode with protection film
JPH06224155A (en) Rf-ecr plasma etching apparatus
JPH06283470A (en) Plasma processing device
JP3499104B2 (en) Plasma processing apparatus and plasma processing method
KR100753868B1 (en) Compound plasma reactor
JPH06342771A (en) Dry etching apparatus
JPH09106900A (en) Plasma processing method and plasma processing device
JP3254069B2 (en) Plasma equipment
JPH1174098A (en) Plasma treatment device
JPH0950898A (en) Plasma treatment device
JPH06232081A (en) Icp plasma processing device
JP2003077904A (en) Apparatus and method for plasma processing
JPH1167725A (en) Plasma etching device
JP3687474B2 (en) Plasma processing equipment
JP3613817B2 (en) Plasma processing equipment
JP3379506B2 (en) Plasma processing method and apparatus
JP3040073B2 (en) Plasma processing equipment
JP3374828B2 (en) Plasma processing method and apparatus