JPH036381A - Microwave plasma processing equipment - Google Patents

Microwave plasma processing equipment

Info

Publication number
JPH036381A
JPH036381A JP1139041A JP13904189A JPH036381A JP H036381 A JPH036381 A JP H036381A JP 1139041 A JP1139041 A JP 1139041A JP 13904189 A JP13904189 A JP 13904189A JP H036381 A JPH036381 A JP H036381A
Authority
JP
Japan
Prior art keywords
substrate
ecr
plasma processing
microwave
wall
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
JP1139041A
Other languages
Japanese (ja)
Other versions
JP2685584B2 (en
Inventor
Takuya Fukuda
福田 琢也
Michio Ogami
大上 三千男
Nobutake Konishi
信武 小西
Tadashi Sonobe
園部 正
Kazuo Suzuki
和夫 鈴木
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.)
HESCO
Hitachi Ltd
Original Assignee
HESCO
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 HESCO, Hitachi Ltd filed Critical HESCO
Priority to JP1139041A priority Critical patent/JP2685584B2/en
Publication of JPH036381A publication Critical patent/JPH036381A/en
Application granted granted Critical
Publication of JP2685584B2 publication Critical patent/JP2685584B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Chemical Vapour Deposition (AREA)
  • Drying Of Semiconductors (AREA)
  • Internal Circuitry In Semiconductor Integrated Circuit Devices (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は電子サイクロトロン共鳴を利用したマイクロ波
プラズマ処理装置に係わり、特にプラズマの処理効率の
向上や、基板への汚染及び異物混入の低減を図るのに好
適なプラズマ処理装置に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a microwave plasma processing apparatus that utilizes electron cyclotron resonance, and is particularly concerned with improving plasma processing efficiency and reducing contamination and foreign matter contamination of substrates. The present invention relates to a plasma processing apparatus suitable for processing.

〔従来の技術〕[Conventional technology]

従来の装置は特開昭62−195124号に記載のよう
に放電管のECR面で生成したプラズマを発散磁界及び
グリッドにより基板処理室内に引き出し、これをホーン
型の金属筒で基板上に均一になるよう流すことで基板を
処理していた。
As described in Japanese Patent Application Laid-Open No. 195124/1984, the conventional apparatus draws plasma generated on the ECR surface of a discharge tube into a substrate processing chamber using a divergent magnetic field and a grid, and then uniformly spreads it onto a substrate using a horn-shaped metal cylinder. The board was processed by flowing it so that it was.

〔発明が解決しようとした課題〕 上記従来技術は、真空容器内壁、導電管、及びグリッド
といった空間中に張り出された物体にプラズマがあたる
ことによって発生する問題について配慮されておらず、
基板汚染や異物発生により適正なデバイス特性を示す半
導体装置の製造がなされなかったり、歩留りが低いとい
った問題があった。
[Problems to be Solved by the Invention] The above-mentioned conventional technology does not take into account the problems that occur when plasma hits objects that extend into space, such as the inner wall of a vacuum container, conductive tubes, and grids.
There have been problems in that due to substrate contamination and the generation of foreign substances, semiconductor devices with appropriate device characteristics cannot be manufactured, and yields are low.

本発明は上記不都合を解決することにある。The present invention aims to solve the above-mentioned disadvantages.

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

本発明は上記目的を達成するために、真空容器内でEC
R条件が満たされる空間のうち、その−部でのみECR
プラズマを発生させることができるようにしたものであ
る。
In order to achieve the above object, the present invention provides EC in a vacuum container.
ECR only in the - part of the space where the R condition is satisfied
It is designed to generate plasma.

また、ECRプラズマの発生を一部の空間に限るため少
なくとも基板処理室空間内にマイクロ波を導波する管を
設置したものである。
Further, in order to limit the generation of ECR plasma to a part of the space, a tube for guiding microwaves is installed at least in the substrate processing chamber space.

さらに、ECRプラズマ発生面をよぎり基板に向う磁力
線を、少なくとも基板上流側で真空容器内壁や導波する
管壁にあたらないようにしたものである。
Furthermore, the magnetic lines of force that cross the ECR plasma generation surface and head toward the substrate are prevented from hitting the inner wall of the vacuum chamber or the wall of the waveguide tube at least on the upstream side of the substrate.

また、上記目的をさらに遂行するため放電管を排除し、
基板処理室内にマイクロ波導波窓を有す3− 4 る構造としたものである。
In addition, in order to further achieve the above purpose, the discharge tube was eliminated,
This structure has a microwave waveguide window inside the substrate processing chamber.

〔作用〕[Effect]

マイクロ波プラズマ装置において、ECRプラズマは、
ECR条件が満たされる磁界強度の空間で、かつ、導入
マイクロ波が導波してくる空間に限定される。また生成
したECRプラズマは磁力線方向に流れる。従って、真
空容器内壁の一部で基板方向側に拡がる領域部、あるい
は真空を維持するため壁面とは異なる領域で容器空間内
の1部にマイクロ波を導波させる領域を作り、該領域部
にECR条件を起こし、かつ該領域をよぎり基板方向に
向う磁力線を、少なくとも基板上流側では、真空容器内
壁等にあたらないようにすると、ECRプラズマ流は生
成位置から基板まで物体にふれることなく基板に到達す
る。このため、容器内壁等を荷電粒子によりスパッタし
たり堆積物を付着させることがなくなり、基板処理の汚
染や異物混入の低減化が著しく図れる。
In the microwave plasma device, the ECR plasma is
It is limited to a space where the magnetic field strength satisfies the ECR conditions and where the introduced microwave is guided. Further, the generated ECR plasma flows in the direction of magnetic field lines. Therefore, a region that extends toward the substrate in a part of the inner wall of the vacuum container, or a region different from the wall surface to maintain vacuum, is created to guide microwaves to a part of the container space. By creating an ECR condition and making sure that the magnetic lines of force that cross the region and head toward the substrate do not hit the inner wall of the vacuum chamber, at least on the upstream side of the substrate, the ECR plasma flow will flow from the generation position to the substrate without touching the substrate. reach. Therefore, sputtering of charged particles or deposition of deposits on the inner wall of the container, etc. is prevented, and contamination of substrate processing and contamination of foreign matter can be significantly reduced.

また、プラズマは、ECR位置だけでなく通常のマイク
ロ波放電によっても生成するので、ECR面とマイクロ
波導入窓の位置は近い方が、上記汚染や異物発生の低減
が図れる。従って、放電管部を排除し、基板処理室内に
マイクロ波導入窓を設置すると、汚染や異物発生はさら
に低減化される。
Further, since plasma is generated not only at the ECR position but also by ordinary microwave discharge, the closer the ECR surface and the microwave introduction window are located, the more the above-mentioned contamination and foreign matter generation can be reduced. Therefore, by eliminating the discharge tube section and installing a microwave introduction window in the substrate processing chamber, contamination and foreign matter generation can be further reduced.

〔実施例〕〔Example〕

以下、本発明を図面を用いて詳細に説明する。 Hereinafter, the present invention will be explained in detail using the drawings.

実施例1゜ 第1図は本発明に基づくマイクロ波プラズマ処理装置の
一型式主要部の断面を示した図である。
Embodiment 1 FIG. 1 is a cross-sectional view of the main part of one type of microwave plasma processing apparatus based on the present invention.

本装置は、マイクロ波導波管1(マイクロ波2の発振機
は図省略)、マイクロ波導入窓3.放電室4、基板5を
処理する処理室6.磁界発生コイル7と8.排気口9(
排気系は図省略)、反応ガスノズル10と11(反応ガ
ス供給系は図省略)、処理室6にマイクロ波を導波する
導波管12よりなる。マイクロ波導入窓3は透明石英製
で、放電室4.処理室6及び導波管12はAQ製である
This device consists of a microwave waveguide 1 (the oscillator for the microwave 2 is not shown), a microwave introduction window 3. A discharge chamber 4, a processing chamber 6 for processing the substrate 5. Magnetic field generating coils 7 and 8. Exhaust port 9 (
(exhaust system is omitted), reaction gas nozzles 10 and 11 (reaction gas supply system is omitted), and a waveguide 12 that guides microwaves into the processing chamber 6. The microwave introduction window 3 is made of transparent quartz, and the discharge chamber 4. The processing chamber 6 and waveguide 12 are made by AQ.

磁界コイル7及び8によりECR位置を図中14bに示
したように導波管12内に位置させることができ、すな
わち処理室6内の空間の一部に制限することかでき、か
つ、ECR面をよぎり基板方向に向う磁力線を図中13
bに示すように導波管12内壁や処理室6の内壁にふれ
ることなく基板に向かわすことができる。この結果、E
CRプラズマ流は図中15bに示すように少なくとも基
板上流側の処理室空間内の物体面にふれることなく基板
に流すことができる。
By means of the magnetic field coils 7 and 8, the ECR position can be located within the waveguide 12 as shown in 14b in the figure, that is, it can be restricted to a part of the space within the processing chamber 6, and the ECR surface can be 13 in the figure shows the lines of magnetic force that cross the
As shown in FIG. 3B, the waveguide can be directed toward the substrate without touching the inner wall of the waveguide 12 or the inner wall of the processing chamber 6. As a result, E
As shown at 15b in the figure, the CR plasma flow can flow onto the substrate without touching at least the object surface in the processing chamber space on the upstream side of the substrate.

本装置を用い、被処理基板として150[mmlφのシ
リコンウェハにシリコン酸化膜、SiO2膜を堆積させ
、堆積膜や堆積表面の異物混入度を調べた。本発明装置
の効果を確める目的で、初めに従来型装置により堆積さ
せた時の状況を調べた。
Using this apparatus, a silicon oxide film and a SiO2 film were deposited on a silicon wafer of 150 mmlφ as a substrate to be processed, and the degree of foreign matter contamination in the deposited film and the deposited surface was examined. In order to confirm the effectiveness of the apparatus of the present invention, we first investigated the situation when depositing with a conventional apparatus.

第2図は従来型装置主要部の断面を示す。第1図に示し
た本発明装置と異なる点は、磁界コイル8がなく、EC
R位置が図中14aに示したように放電管内部に位置し
ていることであり、また磁力線は13aに示したように
放電管部の壁を横ぎるようになっており、ECRプラズ
マ15aのように放電管部内壁にふれている点である。
FIG. 2 shows a cross section of the main parts of a conventional device. The difference from the device of the present invention shown in FIG. 1 is that there is no magnetic field coil 8, and the EC
The R position is located inside the discharge tube as shown at 14a in the figure, and the magnetic field lines cross the wall of the discharge tube section as shown at 13a, and the ECR plasma 15a is This point touches the inner wall of the discharge tube section.

SiO2膜は、第1のガス供給ノズルより酸素、O2を
100 [m Q /m1nl導入し、第2のガス供給
ノズルよりモノシラン、5iHa を20[mn/m1
nl導入し、排気流量を調整することにより処理室6内
の圧力を0.2[Pa]にし、μ波を導入して堆積させ
た。堆積した膜に含まれる異物数は、堆積膜をxps分
析により評価し、堆積膜表面の異物数は面板欠陥装置に
より評価した。堆積膜厚を200 Cn m/m1nl
とし、μ波パワを異ならせた時の膜中に含まれるAQ原
子数を、μ波パワ1000[W]の時の値を100とし
て第2図のAに示す。また、μ波パワ500[W]時で
1枚に200[nm]厚の5iOz膜を堆積させた時の
、表面異物数の処理枚数依存性を第3図のAとして示す
。次に界磁コイル7に流す電流値を上げ、ECR位置を
第2図12とした時のAQ原子数及び表面異物数を第3
図及び第4図のA′として示す。この時の磁力線は第2
図のBa’に示すようにμ波導波管12を横ぎるように
処理室側面に向かっており、この結果ECRプラズマ流
は15a′のように基板上方面で広がっている。次いで
、第7− 1図に示した本発明装置により,磁力線方向以外の条件
は一致させて実験した。その結果を第3図及び第4図の
Bとして示す。第3図及び第4図に示した結果より明ら
かな事は、膜中に混入されるAQ、すなわち装置内壁の
構成材の混入量は及び表面異物数は、ECRプラズマ流
が放電管部からふれるよりは、処理室内の導波管面から
ふれた方、すなわち、プラズマ流がふれる領域が少ない
程、少なく、異物の影響が少ない事がわかる。さらに、
磁力線を制御することでECRプラズマが処理室内の導
波管内部や、少なくとも基板上流側で処理室内壁にふれ
ないようにすると、異物の影響は前述した従来型装置を
用いた時よりも膜の汚染度においては約5〜7倍、表面
異物数においては約10〜15倍少ないことがわかる。
For the SiO2 film, oxygen, O2, was introduced at a rate of 100 [mQ/ml1nl] through the first gas supply nozzle, and monosilane, 5iHa, was introduced at 20[mQ/ml1nl] through the second gas supply nozzle.
nl was introduced, the pressure inside the processing chamber 6 was set to 0.2 [Pa] by adjusting the exhaust flow rate, and μ waves were introduced for deposition. The number of foreign particles contained in the deposited film was evaluated by XPS analysis, and the number of foreign particles on the surface of the deposited film was evaluated using a face plate defect analyzer. Deposited film thickness: 200 Cn m/m1nl
The number of AQ atoms contained in the film when the μ-wave power is varied is shown in A in FIG. 2, with the value at 1000 [W] μ-wave power being 100. Further, when a 5iOz film with a thickness of 200 [nm] is deposited on one film at a μ-wave power of 500 [W], the dependence of the number of surface foreign particles on the number of processed films is shown as A in FIG. Next, increase the current value flowing through the field coil 7, and calculate the number of AQ atoms and the number of surface foreign objects when the ECR position is set to 12 in Figure 2.
It is shown as A' in FIG. At this time, the magnetic field lines are the second
As shown at Ba' in the figure, the ECR plasma flow crosses the μ-wave waveguide 12 toward the side of the processing chamber, and as a result, the ECR plasma flow spreads above the substrate as shown at 15a'. Next, an experiment was conducted using the apparatus of the present invention shown in Fig. 7-1, with the conditions other than the direction of the lines of magnetic force being the same. The results are shown as B in FIGS. 3 and 4. It is clear from the results shown in Figures 3 and 4 that the amount of AQ mixed into the film, that is, the amount of the constituent material of the inner wall of the device, and the number of foreign particles on the surface are affected by the ECR plasma flow coming from the discharge tube. It can be seen that the smaller the area that the plasma flow touches from the waveguide surface in the processing chamber, the less the influence of foreign particles. moreover,
By controlling the magnetic lines of force to prevent the ECR plasma from touching the inside of the waveguide in the processing chamber or at least the walls of the processing chamber on the upstream side of the substrate, the influence of foreign particles can be reduced compared to when using the conventional device described above. It can be seen that the degree of contamination is about 5 to 7 times lower, and the number of foreign substances on the surface is about 10 to 15 times lower.

これらのことにより、ECRプラズマ位置を基板処理内
の空間の一部とし、さらにECRプラズマを基板まで他
の物体にふれることなく流すことを図ると、プラズマに
よる真空容器内壁等をスパッタしたり堆積物を付着させ
たりすることが著しく低減できるため、プラズマ処理時
の基板汚染や異物低減化が図れることがわかる。また、
上記A及びA′の条件での堆積速度は約1 0 0 [
 n m/minコで、速度分布はウェハ内で±12[
%]であったがBの条件ではECRプラズマ流の基板方
向の発散が抑制されたため、堆積速度が約1 5 0 
[ n m /min]となり速度分布は±4[%]と
なった。このことから磁力線方向を制御することでプラ
ズマ流れの効率化と均一化もなされることがわかった。
By making the ECR plasma position a part of the space within the substrate processing and furthermore aiming to flow the ECR plasma to the substrate without touching other objects, it is possible to avoid sputtering or deposits on the inner wall of the vacuum chamber due to the plasma. It can be seen that since it is possible to significantly reduce the amount of adhesion of substances, it is possible to reduce substrate contamination and foreign substances during plasma processing. Also,
The deposition rate under conditions A and A' above is approximately 100 [
n m/min, the velocity distribution within the wafer is ±12[
%], but under condition B, the divergence of the ECR plasma flow toward the substrate was suppressed, so the deposition rate was approximately 150%.
[n m /min], and the speed distribution was ±4 [%]. This indicates that controlling the direction of the magnetic field lines makes the plasma flow more efficient and uniform.

実施例2。Example 2.

被処理基板としてp型シリコン基板(150[IIf1
1]φ)上に熱酸化膜を20 [nm]厚形酸形成後に
多結晶シリコンを300[nm]厚さで堆積し,次にレ
ジストでパターニングした基板を用い、塩素,CQ2ガ
スを用いてエツチングした。
A p-type silicon substrate (150[IIf1
1] After forming a 20 [nm] thick thermal oxide film on φ), deposit polycrystalline silicon to a thickness of 300 [nm], and then using a substrate patterned with resist, using chlorine and CQ2 gas. Etched.

実験は第1のガス供給管より塩素を[、20mQ/mi
nコ導入し、μ波パワ500[Wコ、圧力o.i[Pa
]にて行なった。実験は、装置的には実施例1に示した
A′とBの条件で行った。評価は多結晶シリコンをエツ
チングした後、レジストを除去し、該エツチングで残っ
た多結晶シリコンを電極として、下部シリコン基板との
間の絶縁破壊電界強度を測定することで行なった。条件
A′での8[MV/cm]以上を示す領域は全MO8領
域中57[%コであったが条件Bでは94[%]であっ
た。このことから、ECRプラズマ流を物体にふれさせ
ずに基板へ導入させると、おそらくは、不純物の取り込
み量の違いから、プラズマ処理の適正化が図れることが
わかる。
In the experiment, chlorine was supplied from the first gas supply pipe at a rate of 20 mQ/mi.
n waves were introduced, the μ wave power was 500 [W waves, the pressure was o. i[Pa
]. The experiment was conducted using conditions A' and B shown in Example 1 regarding the apparatus. The evaluation was performed by etching the polycrystalline silicon, removing the resist, using the polycrystalline silicon remaining after the etching as an electrode, and measuring the dielectric breakdown electric field strength between it and the lower silicon substrate. The area showing 8 [MV/cm] or more under condition A' was 57 [%] of the total MO8 area, but under condition B it was 94 [%]. From this, it can be seen that if the ECR plasma flow is introduced into the substrate without touching the object, plasma processing can be optimized, probably due to the difference in the amount of impurities taken in.

実施例3゜ 第5図は本発明にもとづくマイクロ波プラズマ処理装置
の一形態の主要部を示した図である。第1図に示した装
置との違いは、処理室内の導波管の設置のかわりに、マ
イクロ波導入窓3の径より、すなわち放電管部4の径以
上で、かつ、基板設置位置における処理室6c径以下と
した領域12cを形成し、かつ、この領域内にECR1
4cを位置させたことである。この装置を用い、上記条
件以外は実施例のBに示した条件と同じくして5i02
膜を堆積させ、堆積膜に混入されるAfl原子数と表面
異物数を調べた。図中、13c及び14 cは磁力線と
ECR位置を示す。この結果AQ原子混入数は先に示し
たBと同じ値を示したが表面異物数は約10[%]多か
った。これはECRプラズマ生成面で発生した無電荷の
ラジカル種の処理室内壁への付着割合いが、本図に示し
た装置の方が、第1図に示した装置よりも処理室内壁へ
流れ込むのに障害が少なく、このため、処理室内壁への
ラジカル類に堆積が増えたためと考えられる。しかしな
がら、本発明の一形態のようにECRプラズマ生成生成
基波管を特に設置することなく処理室の一部に限定する
ことでも、プラズマ流れを他の物体にふれさせずに基板
へ導入する方法でも、従来型の装置を用いるよりも著し
く異物の影響を避けられることがわがる。
Embodiment 3 FIG. 5 is a diagram showing the main parts of one embodiment of a microwave plasma processing apparatus based on the present invention. The difference with the apparatus shown in FIG. 1 is that instead of installing a waveguide in the processing chamber, the processing A region 12c with a diameter of the chamber 6c or less is formed, and the ECR1 is placed in this region.
4c was positioned. Using this device, the conditions other than the above were the same as those shown in Example B, and
A film was deposited, and the number of Afl atoms mixed into the deposited film and the number of surface foreign substances were investigated. In the figure, 13c and 14c indicate magnetic lines of force and ECR positions. As a result, the number of mixed AQ atoms showed the same value as B shown above, but the number of surface foreign substances was about 10% higher. This is due to the rate at which uncharged radicals generated on the ECR plasma generation surface adhere to the processing chamber wall, but the device shown in this figure has a higher rate of adhesion to the processing chamber wall than the device shown in Fig. 1. This is thought to be due to the fact that there were fewer disturbances in the treatment chamber, and as a result, the amount of radicals deposited on the inner walls of the processing chamber increased. However, as in one embodiment of the present invention, there is a method of introducing the plasma flow to the substrate without touching other objects, even if the ECR plasma generation base wave tube is not particularly installed and is limited to a part of the processing chamber. However, it has been found that the influence of foreign objects can be avoided to a greater extent than when using conventional equipment.

実施例4゜ 第6図は本発明にもとづくプラズマ処理装置の一形態の
主要部断面を示した図である。本装置の特徴は、放電部
を排除し、マイクロ波導入窓を処理室の少なくとも一部
としたことである。この装置1− 2 置を用い、150[mmφ]の基板に15[nm]厚の
ゲート絶縁膜を形成し、その後の工程でnゲートMOS
トランジスターを製造し歩留りを調べた、比較のため、
実施例1に示したA、A’ 、Bの装置条件、実施例3
に示した装置条件をCとして第7図に処理基板板数に対
するMO8製造の歩留りを示す。Dは本装置を用いた結
果を示す。」二記比較条件は、装置条件を異ならせてゲ
ート膜を形成した以外は同一条件とした。この結果から
明らかなように、ECRプラズマを放電部から基板以外
の物体にふれさせた条件(A)では30枚髪超えた所よ
り歩留りO及び処理室内からふれた条件では50枚を超
えたあたりより歩留りOとなるが、ECRプラズマ流が
基板まで物体にふれないで流れる状況(B、C,D)で
は50枚を処理した段階でも歩留りは50%ある。また
、ECR位置で生成したラジカルの処理室内壁にふれる
割合が低い程(BとCの比較)、また、マイクロ波放電
によるプラズマのふれる割合いが低い程(CとDの比較
)、歩留りは高くなることがわかる。
Embodiment 4 FIG. 6 is a cross-sectional view of a main part of an embodiment of a plasma processing apparatus according to the present invention. The feature of this apparatus is that the discharge part is eliminated and the microwave introduction window is made into at least a part of the processing chamber. Using this apparatus 1-2, a 15 [nm] thick gate insulating film was formed on a 150 [mmφ] substrate, and in the subsequent process an n-gate MOS was formed.
For comparison, we manufactured transistors and investigated the yield.
Equipment conditions for A, A', and B shown in Example 1, Example 3
FIG. 7 shows the yield of MO8 production with respect to the number of processed substrates, assuming the apparatus conditions shown in FIG. D shows the results using this device. The conditions for comparison were the same except that the gate film was formed using different device conditions. As is clear from these results, under the condition (A) in which the ECR plasma was brought into contact with an object other than the substrate from the discharge section, the yield was O from the point exceeding 30 sheets, and under the condition (A) in which the ECR plasma was contacted from the processing chamber to an object other than the substrate, it was around 50 sheets. However, in the situation (B, C, D) where the ECR plasma flow flows to the substrate without touching the object, the yield is 50% even when 50 sheets are processed. In addition, the lower the rate of contact of radicals generated at the ECR position with the processing chamber wall (comparison of B and C), and the lower the rate of contact of plasma due to microwave discharge (comparison of C and D), the lower the yield. I know it's going to be expensive.

実施例5゜ 第9図は実施例4に示した装置を大面積の基板を処理で
きるよう、また、処理室内に設置した導波管内でのプラ
ズマスパッタによる異物の低減化を図れるように改善を
図った装置の主要部の断面図を示したものである。処理
室の口径が広くなったことによる装置中心部の印加磁界
の強度低減を防ぐため、磁界コイルには、磁性度の高い
金属板16を被覆し、また、異物、特に金属の基板への
混入を避けるため、導電管12の内壁をシリコン材17
で被覆した。本装置を用い、被処理基板として350[
mm口]のガラス板上にクロム、Cr配線を施しその後
、SiN、ノンドープアモルファスシリコン続いてリン
、Pドープアモルファスシリコンを本装置を用いて形成
し、しかる後に種種の工程を経て液晶デイスプレーを製
造し欠陥発生数を調べた。異物混入の程度の比較をする
ため、第8図に示した被覆膜17を取り除いた装置を用
いて同様の実験をした。前者をE、後者をD′として、
欠陥発生数の基板処理枚数依存性を第9図に示す。この
結果より、シリコン材による被覆を施した装置を用いた
方は、被覆していないものに比して、欠陥発生数が著し
く低いことがわかる。
Embodiment 5 - Figure 9 shows an improvement to the apparatus shown in Embodiment 4 so that it can process large-area substrates and to reduce the amount of foreign matter caused by plasma sputtering in the waveguide installed in the processing chamber. 2 shows a cross-sectional view of the main parts of the device. In order to prevent the strength of the magnetic field applied to the center of the device from decreasing due to the enlarged diameter of the processing chamber, the magnetic field coil is coated with a highly magnetic metal plate 16 to prevent foreign matter, especially metal, from entering the substrate. In order to avoid this, the inner wall of the conductive tube 12 is covered with silicone material
coated with. Using this apparatus, the substrate to be processed is 350 [
After that, SiN, non-doped amorphous silicon, and then phosphorus and P-doped amorphous silicon are formed using this equipment, and then various processes are performed to manufacture a liquid crystal display. The number of defects was investigated. In order to compare the degree of foreign matter contamination, a similar experiment was conducted using the apparatus shown in FIG. 8 from which the coating film 17 was removed. Letting the former be E and the latter D',
FIG. 9 shows the dependence of the number of defects on the number of substrates processed. The results show that the number of defects generated using the device coated with silicon material is significantly lower than that of the device not coated.

このことより、マイクロ波放電により発生するプラズマ
がふれる面にも金属以外の被覆膜を施すことにより、著
しい処理特性の改善が図れることがわかる。
This shows that the processing characteristics can be significantly improved by applying a non-metallic coating to the surface that comes in contact with plasma generated by microwave discharge.

以上、本実施例によれば、マイクロ波プラズマ処理装置
において、ECRプラズマの発生部を真空容器内の一空
間に限定し、かつ、磁力線の向きを制御し、少なくとも
基板上流側で、該ECRプラズマが基板以外の物体にふ
れることなく基板まで流れるようにすると、真空容器内
壁構成材からの基板汚染及び該プラズマによる堆積物の
低減が図れ、半導体装置製造における歩留りの向上が図
れることがわかる。、また上記効果は、ラジカルの流れ
こみゃマイクロ波放電によるプラズマ生成域の低減、及
びプラズマがふれる真空容器壁材質の改善により、さら
に促進されることがわかった。
As described above, according to this embodiment, in the microwave plasma processing apparatus, the ECR plasma generation part is limited to one space in the vacuum container, and the direction of the magnetic field lines is controlled, so that the ECR plasma is generated at least on the upstream side of the substrate. It can be seen that if the plasma is allowed to flow to the substrate without touching objects other than the substrate, contamination of the substrate from the materials constituting the inner wall of the vacuum container and deposits caused by the plasma can be reduced, and the yield in semiconductor device manufacturing can be improved. It has also been found that the above effects are further promoted by reducing the plasma generation area due to the flow of radicals and microwave discharge, and by improving the material of the wall of the vacuum vessel that comes into contact with the plasma.

〔発明の効果〕〔Effect of the invention〕

の低減化が図れるので、半導体装置製造における歩留り
の向」二や信頼性の向上がなされる効果がある。また、
著しく歩留り及び信頼性が高まるので、例えば高解度の
液晶デイスプレーの製造が可能となるといった効果があ
る。
As a result, the yield rate and reliability in semiconductor device manufacturing can be improved. Also,
Since the yield and reliability are significantly increased, it is possible to produce, for example, a high-resolution liquid crystal display.

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

第1図は本発明によるマイクロ波プラズマ処理装置の一
形態を示す図、第2図は従来型装置を示す図、第3図、
第4図は堆積膜へ混入したAQの原子数の相対値比較の
μ波パワ依存性及び基板異物数の処理枚数依存性を示す
図、第5図、第6図。 第8図は本発明装置の一形態を示す図、第7図。 第9図は半導体装置の製造歩留りの処理枚数依存性を示
した図である。 2・・・μ波、4・・・放電部、5・・・基板、6・処
理室、7.8・・磁界コイル、12・・・μ波導波管、
13a−d−磁力線、14 a −e −E CR条件
、15a〜b・・ECRプラズマ領域、16・・金属材
、17シリコン膜、A、A’・・・磁力線制御なし、B
・・・15 ECRプラズマ発生が処理室の導波管内、CECRプラ
ズマが処理室の一部の空間で発生、D・・・放電部なし
、D′・・導波管内壁被覆なし、E導波管内壁の被覆あ
り。
FIG. 1 is a diagram showing one form of a microwave plasma processing apparatus according to the present invention, FIG. 2 is a diagram showing a conventional type apparatus, FIG.
FIG. 4 is a diagram showing the dependence of the relative value of the number of AQ atoms mixed into the deposited film on the μ-wave power, and the dependence of the number of foreign substances on the substrates on the number of processed substrates; FIGS. 5 and 6; FIG. FIG. 8 is a diagram showing one form of the device of the present invention, FIG. FIG. 9 is a diagram showing the dependence of the manufacturing yield of semiconductor devices on the number of processed semiconductor devices. 2...μ wave, 4...discharge section, 5...substrate, 6.processing chamber, 7.8...magnetic field coil, 12...μ wave waveguide,
13a-d-magnetic field lines, 14 a-e-E CR conditions, 15a-b...ECR plasma region, 16...metal material, 17 silicon film, A, A'...no magnetic field line control, B
...15 ECR plasma is generated in the waveguide of the processing chamber, CECR plasma is generated in a part of the processing chamber, D...No discharge part, D'...No waveguide inner wall coating, E waveguide The inner wall of the pipe is covered.

Claims (8)

【特許請求の範囲】[Claims] 1.マイクロ波導入窓、排気系、反応ガス導入系を有し
た真空容器及び電子サイクロトロン共鳴(ECR)を引
き起こすに必要な磁界からなるプラズマ処理装置におい
て、該ECR面で生成した電荷粒子を、被処理基板上流
側にある真空容器側壁及び上流側の空間内に位置した物
体面にふれさせずに基板まで流し、基板を処理すること
を特徴としたマイクロ波プラズマ処理装置。
1. In a plasma processing apparatus consisting of a vacuum vessel having a microwave introduction window, an exhaust system, and a reaction gas introduction system, and a magnetic field necessary to cause electron cyclotron resonance (ECR), the charged particles generated on the ECR surface are transferred to the substrate to be processed. A microwave plasma processing apparatus characterized by processing a substrate by flowing it to the substrate without touching the side wall of the vacuum chamber on the upstream side and an object surface located in the space on the upstream side.
2.上記ECR位置でのプラズマ生成部の、装置中心軸
の垂直方向の径は、マイクロ波導入窓径よりも長く、か
つ、基板位置における真空容器径よりも短いことを特徴
とした特許請求の範囲第1項記載のマイクロ波プラズマ
処理装置。
2. Claim 1, characterized in that the diameter of the plasma generating section at the ECR position in the direction perpendicular to the central axis of the apparatus is longer than the diameter of the microwave introduction window and shorter than the diameter of the vacuum vessel at the substrate position. The microwave plasma processing apparatus according to item 1.
3.上記真空容器が放電管部と基板処理室に分離してい
る装置において、基板処理室の空間の一部に、導入した
マイクロ波を導波させる導波管を設置し、該導電管内に
上記ECRを位置させることを特徴とした特許請求の範
囲第1項又は第2項記載のマイクロ波プラズマ処理装置
3. In an apparatus in which the vacuum vessel is separated into a discharge tube section and a substrate processing chamber, a waveguide for guiding introduced microwaves is installed in a part of the space of the substrate processing chamber, and the ECR 3. The microwave plasma processing apparatus according to claim 1 or 2, wherein:
4.上記ECRによりプラズマを生成させる面をよぎり
、基板方向に向かう磁力線は、基板上流側において、真
空容器内壁や上記導電管内壁にぶつからないことを特徴
とした特許請求の範囲第1項乃至第3項記載のマイクロ
波プラズマ処理装置。
4. Claims 1 to 3 are characterized in that the lines of magnetic force that cross the surface where plasma is generated by the ECR and go toward the substrate do not collide with the inner wall of the vacuum container or the inner wall of the conductive tube on the upstream side of the substrate. The microwave plasma processing apparatus described above.
5.上記基板処理室は放電管部を重ね、マイクロ波導入
窓が基板処理室の基板上方の少なくとも壁面の1部とな
つていることを特徴とした特許請求の範囲第1項乃至第
4項記載のマイクロ波プラズマ処理装置。
5. Claims 1 to 4 are characterized in that the substrate processing chamber has overlapping discharge tube sections, and the microwave introduction window forms at least a part of the wall surface above the substrate of the substrate processing chamber. Microwave plasma processing equipment.
6.少なくとも上記導電管の内壁を、導電管成分と異な
る成分の材質で被覆したことを特徴とした特許請求の範
囲第1項乃至第5項記載のマイクロ波プラズマ処理装置
6. 6. The microwave plasma processing apparatus according to claim 1, wherein at least the inner wall of the conductive tube is coated with a material having a different component from that of the conductive tube.
7.少なくとも磁界コイルの一部を強磁性体でおおうこ
とを特徴としたマイクロ波プラズマ処理装置。
7. A microwave plasma processing device characterized in that at least a part of a magnetic field coil is covered with a ferromagnetic material.
8.特許請求の範囲第1項乃至第7項に記載の装置を用
いた半導体装置の製造を行なうことを特徴とした半導体
装置の製造方法。
8. A method for manufacturing a semiconductor device, comprising manufacturing a semiconductor device using the apparatus according to any one of claims 1 to 7.
JP1139041A 1989-06-02 1989-06-02 Microwave plasma processing equipment Expired - Lifetime JP2685584B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1139041A JP2685584B2 (en) 1989-06-02 1989-06-02 Microwave plasma processing equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1139041A JP2685584B2 (en) 1989-06-02 1989-06-02 Microwave plasma processing equipment

Publications (2)

Publication Number Publication Date
JPH036381A true JPH036381A (en) 1991-01-11
JP2685584B2 JP2685584B2 (en) 1997-12-03

Family

ID=15236078

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1139041A Expired - Lifetime JP2685584B2 (en) 1989-06-02 1989-06-02 Microwave plasma processing equipment

Country Status (1)

Country Link
JP (1) JP2685584B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100724285B1 (en) * 2005-09-13 2007-06-04 주식회사 아이피에스 Plasma treatment device for uniform plasma generation

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH029491U (en) * 1988-06-30 1990-01-22
JPH0361372U (en) * 1989-10-18 1991-06-17

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH029491U (en) * 1988-06-30 1990-01-22
JPH0361372U (en) * 1989-10-18 1991-06-17

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100724285B1 (en) * 2005-09-13 2007-06-04 주식회사 아이피에스 Plasma treatment device for uniform plasma generation

Also Published As

Publication number Publication date
JP2685584B2 (en) 1997-12-03

Similar Documents

Publication Publication Date Title
US5449411A (en) Microwave plasma processing apparatus
US5211825A (en) Plasma processing apparatus and the method of the same
JP3429391B2 (en) Plasma processing method and apparatus
US20010037770A1 (en) Plasma processing apparatus and processing method
JP2602336B2 (en) Plasma processing equipment
EP1119030B1 (en) Plasma reactor
JP3408994B2 (en) Plasma processing apparatus and control method for plasma processing apparatus
JP2595002B2 (en) Microwave plasma processing method and apparatus
JPH036381A (en) Microwave plasma processing equipment
WO2001083852A1 (en) Method and apparatus for distributing gas within high density plasma process chamber to ensure uniform plasma
JPH0415921A (en) Method and apparatus for activating plasma
JP3138899B2 (en) Plasma processing equipment
JP2700890B2 (en) Plasma processing equipment
JP3147769B2 (en) Plasma processing apparatus and processing method
JP2630089B2 (en) Microwave plasma processing equipment
JP3151596B2 (en) Plasma processing method and apparatus
JP3432720B2 (en) Plasma processing apparatus and plasma processing method
JPH07153595A (en) Magnetic field inductively coupled plasma processing system
JPH036380A (en) Microwave plasma processing equipment
JPH0717147Y2 (en) Plasma processing device
JP2539422B2 (en) Plasma CVD flattening film forming method
JPH08302465A (en) Film forming device utilizing sputtering by plasma
JPH08250470A (en) Plasma processing method and processing apparatus
JPS60218826A (en) Formation of thin film
JPH09115880A (en) Dry etching equipment