JPS6017031B2 - plasma etching equipment - Google Patents

plasma etching equipment

Info

Publication number
JPS6017031B2
JPS6017031B2 JP12547082A JP12547082A JPS6017031B2 JP S6017031 B2 JPS6017031 B2 JP S6017031B2 JP 12547082 A JP12547082 A JP 12547082A JP 12547082 A JP12547082 A JP 12547082A JP S6017031 B2 JPS6017031 B2 JP S6017031B2
Authority
JP
Japan
Prior art keywords
plasma etching
electrode
frequency power
cathode
electrodes
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.)
Expired
Application number
JP12547082A
Other languages
Japanese (ja)
Other versions
JPS5916979A (en
Inventor
清 高橋
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.)
Kokusai Electric Corp
Original Assignee
Kokusai Electric Corp
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 Kokusai Electric Corp filed Critical Kokusai Electric Corp
Priority to JP12547082A priority Critical patent/JPS6017031B2/en
Publication of JPS5916979A publication Critical patent/JPS5916979A/en
Publication of JPS6017031B2 publication Critical patent/JPS6017031B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は高周波電力によってプラズマを発生させるプラ
ズマエッチング装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a plasma etching apparatus that generates plasma using high frequency power.

さらに詳しくはホロ‐陰極効果を発生させるカソード電
極を設け、このカソード電極を貫通して吹出す反応ガス
によって強力なエッチングを行なうプラズマエッチング
装置に関するものである。従来プラズマによるエッチン
グではエッチング速度を早くするために電極間に印加す
る高周波電力を増大すると電極間に発生しているセルフ
バイアス電圧も増大し、イオンがはげしく半導体基板へ
衝突して結晶欠陥の原因となる。
More specifically, the present invention relates to a plasma etching apparatus that is provided with a cathode electrode that generates a holo-cathode effect and performs powerful etching with a reactive gas blown out through the cathode electrode. In conventional plasma etching, when the high-frequency power applied between the electrodes is increased in order to increase the etching rate, the self-bias voltage generated between the electrodes also increases, causing ions to violently collide with the semiconductor substrate and cause crystal defects. Become.

またイオンの衝突により発生する熱量も増大し半導体基
板表面の温度上昇がはげしく、この表面をカバーしてい
るマスクが焼けるという問題がある。またェポキシ樹脂
の多層積層の配線板の場合、′ドリルによる孔あげ後、
孔の側壁に残る切粉や、孔あげ作業後孔の側壁に露出す
べき中間層の導体膜がドリルとの摩擦熱によって切粉が
融着してカバーされてしまうことがある。
Furthermore, the amount of heat generated by the collision of ions also increases, causing a sharp rise in temperature on the surface of the semiconductor substrate, causing a problem that the mask covering this surface may be burnt. In addition, in the case of a multilayer laminated wiring board made of epoxy resin, after drilling holes,
Chips remaining on the side wall of the hole or the conductive film of the intermediate layer that should be exposed on the side wall of the hole after drilling may be fused and covered by the frictional heat from the drill.

これらの切粉や融着性を除去するためにプラズマによる
エッチングを行っても孔の中間部はエッチングされにく
いという問題がある。本発明はこれらの問題を解決する
ためになされたもので、半導体基板に対しては結晶欠陥
を起すことなく、またェポキシ樹脂の多層積層の配線板
に対しては細いドリル孔の内部まで完全にエッチング出
来るエッチング装置を提供するものである。
Even if plasma etching is performed to remove these chips and fusion properties, there is a problem in that the intermediate portion of the hole is difficult to be etched. The present invention has been made to solve these problems, and it can be used without causing crystal defects for semiconductor substrates, and completely to the inside of thin drill holes for multilayer wiring boards made of epoxy resin. An etching device capable of etching is provided.

以下図面により詳細に説明する。This will be explained in detail below with reference to the drawings.

構造説明の前にホロー陰極効果について説明する。Before explaining the structure, the hollow cathode effect will be explained.

陰極形状を2個以上のU字形あるいは円筒形とし、これ
らの間にそれぞれの陰極面から一定の所に負のグロー放
電が現われるようにした陰極をホロ−陰極という。この
2個以上の陰極間隔を適当値に選ぶか、ガス圧を適当値
に選ぶとそれぞれの陰極側の負のグロー放電が合体して
一つのグロー放電となる。これをホロー陰極効果という
。このようにするとグロー放電の維持電圧が低下する反
面、陰極電流密度が飛躍的に増加する。本発明はこの原
理を応用したものである。第1図は互に対向する電極の
片方にのみホロ−陰極効果を持たせたもので、前記の半
導体基板のエッチングに適した装置の主要な構成を示す
ものである。
A cathode having two or more U-shaped or cylindrical cathodes in which a negative glow discharge appears at a fixed location from each cathode surface is called a holo-cathode. If the distance between these two or more cathodes is selected to an appropriate value, or if the gas pressure is selected to an appropriate value, the negative glow discharges on each cathode side are combined to form one glow discharge. This is called the hollow cathode effect. In this case, the sustaining voltage of the glow discharge decreases, but the cathode current density increases dramatically. The present invention applies this principle. FIG. 1 shows the main structure of an apparatus suitable for etching a semiconductor substrate as described above, in which only one of the mutually opposing electrodes has a holo-cathode effect.

ここで1は陽極、2はホロー陰極効果を持った陰極、3
はコンデンサ、4は高周波電源、5は被エッチング物で
ある。高周波電源を動作させると互に対向する電極間に
高周波電界が発生するので、この間にあるガス分子は電
離してイオンと電子に分かれる。この場合電子は質量が
極めて軽いので高周波電界の速い変化に対応して各時点
でプラス側の電極に殺到してしまうが、イオンは質量が
大きいので、高周波電界の速い変化に応じ切れずに中間
に滞留してしまう。この場合、電極(陽極)1は接地さ
れているので常にゼロ電位であるが、電極(陰極)2に
到達した電子はコンデンサ3にチャージされてしまうの
で、電極2は負電位となって陰極を形成し、前記陽極1
との間にセルフバイアス電圧が発生する。なお、ホロー
陰極効果を持させるための陰極の構造に関しては後述す
る。第2図は互に対向する電極の両方にホロ−陰極効果
を持たせたもので、第1図との大きな相異点はそれぞれ
の電極と接地間にコンデンサと高周波電源とを別個に接
続してある。
Here, 1 is an anode, 2 is a cathode with a hollow cathode effect, and 3 is a cathode with a hollow cathode effect.
4 is a capacitor, 4 is a high frequency power supply, and 5 is an object to be etched. When a high-frequency power source is operated, a high-frequency electric field is generated between the electrodes facing each other, and gas molecules between the electrodes are ionized and separated into ions and electrons. In this case, since electrons have extremely light mass, they respond to rapid changes in the high-frequency electric field and rush to the positive electrode at each point, but ions have large mass, so they cannot respond to rapid changes in the high-frequency electric field and It stays in. In this case, electrode (anode) 1 is grounded, so it is always at zero potential, but the electrons that reach electrode (cathode) 2 are charged in capacitor 3, so electrode 2 becomes negative potential and connects the cathode. forming the anode 1
A self-bias voltage is generated between Note that the structure of the cathode for providing the hollow cathode effect will be described later. Figure 2 shows a holo-cathode effect on both electrodes facing each other, and the major difference from Figure 1 is that a capacitor and a high-frequency power source are connected separately between each electrode and ground. There is.

このようにすると互に他の側の高周波電源の位相とは関
係ないこ前記説明のようにそれぞれの電極が陰極を形成
し、前記のようなホロー陰極効果を持つ。この実施例は
前記のェボキシ樹脂の多層積層の配線板のドリル孔の内
部エッチングに適するもので、孔の両側からエッチング
が進行する。第3図はホロー陰極効果を持ったエッチン
グ菱贋の反応室部分の断面図で、第1図の場合に相当す
る。
In this way, each electrode forms a cathode as described above, regardless of the phase of the high frequency power source on the other side, and has the hollow cathode effect as described above. This embodiment is suitable for internal etching of a drilled hole in a multi-layer wiring board made of epoxy resin, and etching proceeds from both sides of the hole. FIG. 3 is a cross-sectional view of a reaction chamber portion of an etched diamond plate having a hollow cathode effect, and corresponds to the case of FIG. 1.

図において、1は陽極、2−1は陰極2の一部分の電極
棒である。この陰極2は第4図に示すように複数の電極
棒2−1、接続板2−2、高周波電力導入端子2−3よ
りなるものである。5は被エッチング物、6は真空容器
、7はガス導入口、8はガス吹出口で、互に隣接する前
記電極綾2−1の中間に設けられており、列をなした複
数の孔でも良いし、1本の最孔でも良い。
In the figure, 1 is an anode, and 2-1 is an electrode rod that is part of the cathode 2. As shown in FIG. 4, this cathode 2 consists of a plurality of electrode rods 2-1, a connecting plate 2-2, and a high-frequency power introduction terminal 2-3. 5 is an object to be etched, 6 is a vacuum container, 7 is a gas inlet, and 8 is a gas outlet, which are provided between the adjacent electrodes 2-1, and even if a plurality of holes are arranged in a row. It's fine, and just one hole is fine.

9はガス排出口、10はガス室である。9 is a gas exhaust port, and 10 is a gas chamber.

真空容器6の内部にガス導入口7から反応ガスを導入し
、ガス排出口9から図示してない排気ポンプで排気して
反応ガスの導入量と排出量を調節すれば真空容器6の内
部は一定の減圧状態の反応ガス雰囲気とすることが出来
る。
By introducing a reaction gas into the vacuum container 6 from the gas inlet 7 and exhausting it from the gas exhaust port 9 with an exhaust pump (not shown) to adjust the amount of introduction and discharge of the reaction gas, the inside of the vacuum container 6 can be It is possible to create a reaction gas atmosphere in a constant reduced pressure state.

しか導入される反応ガスはガス室10からガス吹出口8
を通って真空容器Sの内部に吹出すので、この吹出す遍
路は陰極2の電極榛2−1の間を通過することになる。
ここで高周波電源をオンにして、陽極1と陰極2とに高
周波電力を印加すると前記説明のように陰極2の電極棒
2−1の間に負のグロー放電が発生する。
Only the reaction gas introduced is from the gas chamber 10 through the gas outlet 8.
Since the air is blown out into the interior of the vacuum container S through the air, the path of this blown air passes between the electrode fins 2-1 of the cathode 2.
When the high frequency power source is turned on and high frequency power is applied to the anode 1 and the cathode 2, a negative glow discharge is generated between the electrode rods 2-1 of the cathode 2 as described above.

この場合これらのグロー放電がそれぞれの電極棒2一1
の間でそれぞれ1個所に合体するように電極榛2一1の
間隔を調節しておくか、もしくは真空容器内の圧力を調
節すれば、前記合体したグロー放電により濃密なイオン
が発生する。このために高周波電力を増大しなくても単
なる平行平板電極の場合よりはるかに多量のイオンが発
生するものである。しかも高周波電力を増大しないので
、これに伴う前記セルフバイアス電圧は増大せず、イオ
ンの移動速度が増大しないので陰極2と陽極1の中間も
しくは陽極面上に置かれた被エッチング物5であるが半
導体基板に結晶欠陥を発生させることがない。なお、図
示された陽極1は反応ガスをガス排出口9から排出する
ために小孔をあげたものであるが、中央部または周辺部
に反応ガスの通路を設けたものでも良い。この実施例で
の陰極は第4図に示すように構造は簡単であるが、各電
極棒2一1の先端は自由端となって接続されていないの
で、印加する高周波電力の周波数が高いと電極内のィン
ダクタンス分によって同一電極内でも電位差を生じる。
In this case, these glow discharges
If the spacing between the electrode fins 2 and 1 is adjusted so that they are combined at one place between the electrodes, or if the pressure inside the vacuum container is adjusted, dense ions are generated by the combined glow discharge. For this reason, even without increasing the high frequency power, a much larger amount of ions is generated than in the case of a simple parallel plate electrode. Moreover, since the high-frequency power is not increased, the self-bias voltage accompanying this does not increase, and the moving speed of ions does not increase. No crystal defects are generated in the semiconductor substrate. Although the illustrated anode 1 has small holes for discharging the reactive gas from the gas outlet 9, it may also have a passageway for the reactive gas in the center or the periphery. The structure of the cathode in this embodiment is simple as shown in FIG. 4, but since the tips of each electrode rod 2-1 are free ends and are not connected, if the frequency of the applied high-frequency power is high, A potential difference occurs even within the same electrode due to inductance within the electrode.

この結果、電位の高い所からアーク放電を起すことがあ
るので、あまり高い周波数の場合には使用出釆ない。第
5図は他の実施例で第3図および第4の陰極部分が異る
ものである。
As a result, arc discharge may occur from places with high potential, so it cannot be used at very high frequencies. FIG. 5 shows another embodiment in which the cathode portions shown in FIG. 3 and 4 are different.

すなわち電極漣2一1、接続板2−2、高周波電力導入
耐子2−3、ガス導入口7、ガス吹出口8およびガス室
10を一体構造として陰極を形成したものである。この
ために前記の電極棒2−1の代りに陽極1に対向する面
に互に平行な複数本の突堤2−4を設け、隣接する突堤
2−4との間の部分に列をなした複数の小孔もしくは1
本の長孔のガス吹出口8を設けたものである。このこと
により両軍極1および2に高周波電力を印加すると、前
記突堤2一4の相互間に強力なグロー放電が発生して大
量のイオンが供給される。しかもこの陰極2は一体構造
であるために電極内のィンダクタンス分は小さく、前記
のような電極内の電位差は4・さし、ので、アーク放電
が起らず、高い周波数の場合でも使用出来る。このよう
に、本発明の装置ではイオンの発生量を増してエッチン
グ速度を早めるために印加する高周波電力を高めないの
で、この結果セルフバイアス電圧が増大してイオンの運
動エネルギーが増大せず。結晶欠陥が起らない。またェ
ポキシ樹脂の多層積層の配線板のような場合は被エッチ
ング物の両面から同時にエッチング出来るので、作業時
間を短縮する効果もある。なお、本発明の装置ではホロ
ー陰極効果により大量のイオンを発生出来るが、このホ
ロー陰極効果は陰極面全域に発生するものではない。
That is, the cathode is formed by integrating the electrode rim 2-1, the connecting plate 2-2, the high-frequency power introduction shield 2-3, the gas inlet 7, the gas outlet 8, and the gas chamber 10. For this purpose, in place of the electrode rod 2-1, a plurality of parallel jetties 2-4 were provided on the surface facing the anode 1, and a row was formed between the adjacent jets 2-4. multiple small holes or one
A gas outlet 8 in the form of a long hole is provided. As a result, when high-frequency power is applied to both military poles 1 and 2, a strong glow discharge is generated between the jetties 2 and 4, and a large amount of ions are supplied. Moreover, since this cathode 2 has a monolithic structure, the inductance within the electrode is small, and the potential difference within the electrode as described above is 4 mm, so arc discharge does not occur and it can be used even at high frequencies. . As described above, in the apparatus of the present invention, the applied high frequency power is not increased in order to increase the amount of ions generated and speed up the etching rate, so as a result, the self-bias voltage does not increase and the kinetic energy of the ions does not increase. No crystal defects occur. Furthermore, in the case of a wiring board made of multi-layered epoxy resin, etching can be performed from both sides of the object at the same time, which has the effect of shortening the working time. Note that although the device of the present invention can generate a large amount of ions due to the hollow cathode effect, this hollow cathode effect is not generated over the entire cathode surface.

0 このため、被エッチング物は場所により多少エッチ
ング速度のバラッキが存在するが、これに対しては被エ
ッチング物を回転や移動などさせれ‘よ容易に均一化す
ることが出来る。
0 For this reason, there is some variation in the etching rate depending on the location of the object to be etched, but this can be easily made uniform by rotating or moving the object to be etched.

以上のよう本発明の装置では従釆の問題点を解夕決する
ばかりでなく、さらに進んで作業時間の短緒などの効果
もあるので、実用上極めて有効である。
As described above, the apparatus of the present invention not only solves the problems of the conventional method, but also has the effect of shortening the working time, so it is extremely effective in practice.

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

第1図および第2図は本発明の装置の動作原理0を説明
する説明図、第3図は本発明の一実施例反応室部分の断
面図、第4図は第3図の場合の陰極の外観図、第5図は
本発明の他の実施例の反応室部分の断面図である。 図において、1は陽極、2は陰極、3はコンデタンサ、
4は高周波電源、5は被エッチング物である。 第1図r 第2図 !第3図 第4図 第5図
1 and 2 are explanatory diagrams explaining the operating principle 0 of the apparatus of the present invention, FIG. 3 is a sectional view of a reaction chamber portion of an embodiment of the present invention, and FIG. 4 is a cathode in the case of FIG. 3. FIG. 5 is a sectional view of the reaction chamber portion of another embodiment of the present invention. In the figure, 1 is an anode, 2 is a cathode, 3 is a capacitor,
4 is a high frequency power source, and 5 is an object to be etched. Figure 1 r Figure 2! Figure 3 Figure 4 Figure 5

Claims (1)

【特許請求の範囲】 1 高周波電力によつてプラズマを発生させるプラズマ
エツチング装置において、互に対向する電極のうち片方
はホロー陰極効果を表わす手段を設けた電極とし、この
電極をコンデンサおよび高周波電源を介して接地し、前
記互に対向する電極のうち他方は直接接地し、前記ホロ
ー陰極効果を表わす手段の間に反応ガス吹出口を設けて
構成したことを特徴とするプラズマエツチング装置。 2 高周波電力によつてプラズマを発生させるプラズマ
エツチング装置において、互に対向する電極の両方とも
ホロー陰極効果を表わす手段を設けた電極とし、これら
両方の電極を各別にコンデンサおよび高周波電源を介し
て接地し、前記それぞれの電極のホロー陰極効果を表わ
す手段の間に反応ガス吹出口を設けて構成したことを特
徴とするプラズマエツチング装置。 3 特許請求の範囲第1項および第2項のうちの1つに
記載されたプラズマエツチング装置において、ホロー陰
極効果を表わす手段を設けた電極として平行で等間隔に
配列した複数の電極棒と、これらの電極棒の一端をそれ
ぞれ連結する接続板とより構成したことを特徴とする前
記プラズマエツチング装置。 4 特許請求の範囲第1項および第2項のうちの1つに
記載されたプラズマエツチング装置において、ホロー陰
極効果を表わす手段を設けた電極として中空構造で他方
の電極に対向する面に等間隔で互に平行する複数の突堤
を設け、これらの突堤相互間の底部にガス吹出口を設け
、他方の電極に対向する面と反対側の面にガス導入口を
設けて構成したことを特徴とする前記プラズマエツチン
グ装置。
[Claims] 1. In a plasma etching device that generates plasma using high-frequency power, one of the opposing electrodes is provided with a means for expressing a hollow cathode effect, and this electrode is connected to a capacitor and a high-frequency power supply. A plasma etching apparatus characterized in that the other of the mutually opposing electrodes is directly grounded, and a reactive gas outlet is provided between the hollow cathode effect means. 2. In a plasma etching device that generates plasma using high-frequency power, both of the electrodes facing each other are provided with means for expressing a hollow cathode effect, and both electrodes are individually grounded via a capacitor and a high-frequency power source. A plasma etching apparatus characterized in that a reactive gas outlet is provided between the means for expressing the hollow cathode effect of each of the electrodes. 3. A plasma etching apparatus according to one of claims 1 and 2, including a plurality of electrode rods arranged in parallel and at equal intervals as electrodes provided with means for expressing a hollow cathode effect; The plasma etching apparatus is characterized in that it comprises a connecting plate that connects one end of each of these electrode rods. 4. In the plasma etching apparatus according to one of claims 1 and 2, the electrode is provided with a means for expressing a hollow cathode effect, which has a hollow structure and is arranged at equal intervals on the surface facing the other electrode. A plurality of jetties are provided parallel to each other, a gas outlet is provided at the bottom between these jetties, and a gas inlet is provided on the surface opposite to the surface facing the other electrode. The plasma etching apparatus.
JP12547082A 1982-07-19 1982-07-19 plasma etching equipment Expired JPS6017031B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12547082A JPS6017031B2 (en) 1982-07-19 1982-07-19 plasma etching equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12547082A JPS6017031B2 (en) 1982-07-19 1982-07-19 plasma etching equipment

Publications (2)

Publication Number Publication Date
JPS5916979A JPS5916979A (en) 1984-01-28
JPS6017031B2 true JPS6017031B2 (en) 1985-04-30

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP12547082A Expired JPS6017031B2 (en) 1982-07-19 1982-07-19 plasma etching equipment

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Country Link
JP (1) JPS6017031B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4521286A (en) * 1983-03-09 1985-06-04 Unisearch Limited Hollow cathode sputter etcher
JPS61272928A (en) * 1985-05-29 1986-12-03 Ulvac Corp Dryetching process
US4637853A (en) * 1985-07-29 1987-01-20 International Business Machines Corporation Hollow cathode enhanced plasma for high rate reactive ion etching and deposition

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