JPS63219579A - Sputtering device - Google Patents

Sputtering device

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Publication number
JPS63219579A
JPS63219579A JP5270687A JP5270687A JPS63219579A JP S63219579 A JPS63219579 A JP S63219579A JP 5270687 A JP5270687 A JP 5270687A JP 5270687 A JP5270687 A JP 5270687A JP S63219579 A JPS63219579 A JP S63219579A
Authority
JP
Japan
Prior art keywords
intermediate electrode
sputtering
targets
space
target
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
JP5270687A
Other languages
Japanese (ja)
Other versions
JP2580149B2 (en
Inventor
Masahiko Naoe
直江 正彦
Yoichi Hoshi
陽一 星
Yasuhiro Sakai
康裕 酒井
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.)
OSAKA SHINKU KIKI SEISAKUSHO KK
Original Assignee
OSAKA SHINKU KIKI SEISAKUSHO KK
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 OSAKA SHINKU KIKI SEISAKUSHO KK filed Critical OSAKA SHINKU KIKI SEISAKUSHO KK
Priority to JP62052706A priority Critical patent/JP2580149B2/en
Publication of JPS63219579A publication Critical patent/JPS63219579A/en
Application granted granted Critical
Publication of JP2580149B2 publication Critical patent/JP2580149B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To sputter-etching the sputtered particles deposited on an intermediate electrode at a low rate and improve the efficiency in forming a thin film, by using the intermediate electrode facing the magnetic field space between inner and outer targets as the cathode at a voltage lower than both targets. CONSTITUTION:The annular outside target 4a with the inner peripheral side facing a sputtering surface 12 as the sputtering surface 12a is arranged around the inside target 4 with the outer peripheral side as the sputtering surface 12. The magnetic field space 7 wherein plasma is produced when both targets 4 an 4a are sputtered is formed between both sputtering surfaces 12 and 12a. In the sputtering device of such a structure, the intermediate electrode 6 is provided on the rear sides of the targets 4 and 4a and opposed to the magnetic field space 7. In addition, the intermediate electrode 6 is used as the cathode at a voltage lower than both targets 4 an 4a, and sputter-etching is carried out at a rate lower than the rate at which the sputtered particles generated in the space 7 are deposited on the intermediate electrode 6. By this method, the deposition and absorption of the sputtered particles are prevented, and the efficiency in forming the specified thin film is improved.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は磁気記録媒体の製造の如き強磁性体等の薄膜生
成手段に用いられるスパッタ装置に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a sputtering apparatus used for producing a thin film of ferromagnetic material or the like in the production of magnetic recording media.

(従来の技術) 従来、この種スパッタ作業としては、第3図に示す様な
もの(例えば特開昭61−284573号所載の装置)
が開発されるに至っている。
(Prior Art) Conventionally, this type of sputtering work has been carried out using a method as shown in FIG.
has been developed.

すなわち、同図に示すものは、平面円形リング状の内側
ターゲット4と外側ターゲット4aとを同心状に配置せ
しめて、両ターゲット4.4aの各スパッタ面12.1
2a間の磁界空間部7内にプラズマ空間を発生させるも
のである。
That is, in the case shown in the same figure, an inner target 4 and an outer target 4a each having a planar circular ring shape are arranged concentrically, and each sputtering surface 12.1 of both targets 4.4a is arranged concentrically.
A plasma space is generated in the magnetic field space section 7 between the magnetic field parts 2a and 2a.

従って、該手段によればターゲット4.4aの配置態様
が従来の所謂平板マグネトロンスパッタ装置と同様とな
って装置構成の簡略化が図れ、またそのスパッタ作業は
従来の対向ターゲット式スパッタ装置と同様な原理によ
り低圧スパッタガス雰囲気内で効率良く行え、しかもタ
ーゲットの利用効率が向上するという利点が得られる。
Therefore, according to this means, the arrangement of the targets 4.4a is similar to that of the conventional so-called flat plate magnetron sputtering apparatus, which simplifies the apparatus configuration, and the sputtering operation is similar to that of the conventional facing target type sputtering apparatus. Based on the principle, sputtering can be performed efficiently in a low-pressure sputtering gas atmosphere, and the advantage is that target utilization efficiency is improved.

然して、前記の型式の装置に於いては、プラズマが発生
される空間部7に対して第4図の如くバッキングプレー
ト1を直面させておけば、ターゲット4.4aと同電位
にあるバッキングプレート1がら空間部7内へ放出され
る二次電子がEXBドリフト移動しながらバッキングプ
レート1の表面付近に閉込められて、その付近のプラズ
マ密度を高めてしまうために、バッキングプレート1自
体が通常のマグネトロンスパッタと同様な原理でスパッ
タされる現象が生じ、その結果績バッキングプレート1
の材料成分が基板13の表面の生成膜中に混入されて生
成薄膜の品質の低下を来たす難点が生じる。
However, in the above type of apparatus, if the backing plate 1 is made to face the space 7 where plasma is generated as shown in FIG. 4, the backing plate 1 at the same potential as the target 4.4a Secondary electrons emitted into the space 7 are trapped near the surface of the backing plate 1 while moving through the EXB drift, increasing the plasma density in the vicinity. A sputtering phenomenon occurs based on the same principle as sputtering, and as a result, the backing plate 1
A problem arises in that the material components are mixed into the formed film on the surface of the substrate 13, resulting in a deterioration in the quality of the formed thin film.

従って、従来に於いては前記難点を解消するために、先
の第3図の如くターゲット4.4a間の空間部7の下方
にスパッタを不可とするアノード20を設ける手段が採
用されていた。
Therefore, in the past, in order to solve the above-mentioned drawbacks, a method was adopted in which an anode 20 that prevents sputtering was provided below the space 7 between the targets 4 and 4a, as shown in FIG.

(発明が解決しようとする問題点) しかるに、前記従来の手段に終いては、バッキングプレ
ート1のスパッタ浸食を防止する策としてアノード20
(陽極)を設けてなるために、該アノード20には空間
部7内に発生せしめたプラズマ内のスパッタ粒子、即ち
ターゲット原子等が一方的に付着、堆積するという無駄
な現象が生じる。
(Problems to be Solved by the Invention) However, in the conventional means, as a measure to prevent sputter erosion of the backing plate 1, the anode 20 is
(anode), a wasteful phenomenon occurs in which sputtered particles, ie, target atoms, etc. in the plasma generated in the space 7 are unilaterally attached and deposited on the anode 20.

従って、従来では前記の様な現象の下、スパッタせしめ
たターゲット原子を空間部7の外方側の基板13に対し
て効率良(付着させることができないこととなり、所定
の薄膜生成作業の効率低下を来すという問題点を有して
いたのである。
Therefore, conventionally, under the above-mentioned phenomenon, the sputtered target atoms cannot be efficiently attached to the substrate 13 on the outside of the space 7, resulting in a decrease in the efficiency of the predetermined thin film production operation. This had the problem of causing

本発明は上記の如き従来の問題点に鑑みて考案されたも
ので、その目的とするところは、バッキングプレート等
の不当なスパッタ現象を防止させるに際して、両ターゲ
ット間の空間部内に発生せしめたスパッタ粒子がターゲ
ットの背面側に設けられた部材に対して一方的に付着、
吸収される様な無駄な現象を生じさせることなく、スパ
ッタ作業による所定の薄膜生成効率を向上させる点にあ
る。
The present invention has been devised in view of the above-mentioned conventional problems, and its purpose is to prevent spatter generated in the space between both targets in order to prevent unreasonable sputtering from the backing plate, etc. Particles unilaterally adhere to the member provided on the back side of the target,
The purpose of this method is to improve the efficiency of forming a predetermined thin film by sputtering without causing wasteful phenomena such as absorption.

(問題点を解決するための手段) 本発明は従来のアノード電極に代えてカソード(陰極)
を採用して、該電極部分に一方的に付着されていたスパ
ッタ粒子を積極的にスバ・ツタさせて該スパッタ粒子を
薄膜生成に利用させることにより、上記従来の問題点を
解決せんとして構成されたものである。
(Means for Solving the Problems) The present invention provides a cathode electrode instead of a conventional anode electrode.
This method is designed to solve the above-mentioned conventional problems by actively causing the sputtered particles that have been unilaterally attached to the electrode part to splatter and to use the sputtered particles for forming a thin film. It is something that

すなわち、本発明の構成の要旨は、両ターゲ・ノド4.
4aの背面部側から磁界空間部7に対面させた状態で設
けた中間電極6を、前記空間部7に発生される空間プラ
ズマのスパッタ粒子が該中間電極6に付着する速度より
も低速のスパッタが行われるべく前記両ターゲット4.
4aよりも低電圧の陰極として構成した点にある。
That is, the gist of the configuration of the present invention is that both targets and throat 4.
The intermediate electrode 6, which is provided facing the magnetic field space 7 from the rear side of 4a, is sputtered at a speed lower than the speed at which the sputtered particles of the spatial plasma generated in the space 7 adhere to the intermediate electrode 6. Both targets 4.
The point is that it is configured as a cathode with a lower voltage than 4a.

(作用) すなわち、上記構成を特徴とするスパッタ装置・に於い
ては、両ターゲット4.4aのスパッタによって磁界空
間部7内に発生されたターゲット4.4aのスパッタ粒
子の一部が中間電極6の表面部に付着することとなるが
、一方該中間電掻6はスパッタ現象を生じてその表面に
付着されたスパッタ粒子を再スパツタするために、該ス
バ・ツタ粒子は再度空間部7内に放出され、これによっ
て所定の薄膜生成速度が高速で行われることとなる。
(Function) That is, in the sputtering apparatus characterized by the above configuration, some of the sputtered particles of the target 4.4a generated in the magnetic field space 7 by the sputtering of both targets 4.4a are transferred to the intermediate electrode 6. On the other hand, since the intermediate electric scraper 6 causes a sputtering phenomenon and re-sputters the sputtered particles attached to its surface, the sputtered particles are once again deposited into the space 7. This results in a high predetermined thin film formation rate.

尚、中間電極60表面部のスパッタ浸食速度は、空間部
7側から中間電極6の表面にスパッタ粒子が付着する速
度よりも小さいために、中間電極6自体の材料成分がス
パッタされて空間部7内に放出される様なことはない。
Incidentally, since the sputter erosion rate of the surface of the intermediate electrode 60 is lower than the rate at which sputter particles adhere to the surface of the intermediate electrode 6 from the space 7 side, material components of the intermediate electrode 6 itself are sputtered and There is no such thing as being released inside.

また、前記中間電極6側のスパッタ現象によって該中間
電極6から放出される二次電子は中間電極6の表面上を
EXBドリフトで移動してスバフタガスのイオン化を促
進するために、これによって磁界空間部7内のプラズマ
密度が一層高くなる作用をも生じる。
Further, the secondary electrons emitted from the intermediate electrode 6 due to the sputtering phenomenon on the intermediate electrode 6 side move on the surface of the intermediate electrode 6 by EXB drift to promote ionization of the buffing gas. This also results in the effect that the plasma density within 7 becomes even higher.

(実施例) 以下、本発明の実施例について図面を参照して説明する
(Example) Hereinafter, an example of the present invention will be described with reference to the drawings.

第1図に於いて、1.1aは両者間にリング状の溝部2
を形成すべく同心状に設けられた銅製等の一対のバッキ
ングプレートを示し、中央部側のプレー)1は上部閉塞
状の略円筒状に形成され、又他方のプレートla側は中
空円板状である。3.3aは前記プレート1.1aの各
表面上に設けられた円柱状の内側ヨーク並びにリング状
の外側ヨークを夫々示す。
In Figure 1, 1.1a is a ring-shaped groove 2 between the two.
The figure shows a pair of backing plates made of copper or the like that are concentrically provided to form a backing plate, in which the central plate (1) is formed into a substantially cylindrical shape with a closed top, and the other plate (la) is shaped like a hollow disk. It is. 3.3a shows a cylindrical inner yoke and a ring-shaped outer yoke provided on each surface of the plate 1.1a.

4.4aは夫々大きさの異なる円形リング状に形成され
た強磁性体等からなる一対のターゲットを示し、一方の
内側ターゲット4は内側ヨーク3の外周に嵌合され、又
他方の外側ターゲット4aは外側ヨーク3aの内周側に
嵌合されて各バッキングプレート1、laの表面上に取
付けられてなる。7は前記内側ターゲット4の外周のス
パッタ面12と外側ターゲット4aの内周のスパッタ面
12aとの両者間に形成された空間部を示し、該空間部
7には磁石9.9a、9bによって各スパッタ面12.
12aと略直交する方向の磁界(例えば2700e、)
が形成されている。11はバッキングブレー)ISla
の下方に別途設けられたヨークを示し、該ヨーク11に
は前記両ターゲット4.4aを陰極とすぺ(電圧を印加
するための電圧可変の電源15が接続されている。
4.4a shows a pair of targets made of ferromagnetic material or the like formed into circular ring shapes of different sizes, one inner target 4 fitted on the outer periphery of the inner yoke 3, and the other outer target 4a is fitted onto the inner peripheral side of the outer yoke 3a and attached to the surface of each backing plate 1, la. Reference numeral 7 designates a space formed between the sputtering surface 12 on the outer periphery of the inner target 4 and the sputtering surface 12a on the inner periphery of the outer target 4a. Sputter surface 12.
A magnetic field in a direction substantially perpendicular to 12a (for example, 2700e)
is formed. 11 is the backing brake) ISla
A variable voltage power source 15 for applying a voltage is connected to the yoke 11, with both targets 4.4a serving as cathodes.

6は前記バッキングブレー)11aの両者間の溝部2内
に位置してその上端面が空間部7と対面すべくボルト等
によって絶縁体14を介して取付けられた中間電極を示
し、該中間電極6は前記ターゲット4.4aへの印加電
圧よりも低い負の電圧が印加されるべく前記電源15と
電圧調整手段16を介して接続されている。
Reference numeral 6 indicates an intermediate electrode which is located in the groove 2 between the backing brakes 11a and is attached via an insulator 14 with bolts or the like so that its upper end face faces the space 7. is connected to the power source 15 via voltage adjustment means 16 so that a negative voltage lower than the voltage applied to the target 4.4a is applied thereto.

5.5aは前記ヨーク3.3aを覆設すべく各ヨーク3
.3aの外方に設けられたグランドシールド板を示し、
該シールド板5.5aはヨーク3.3aやバッキングブ
レートIa等とは絶縁された状態で接地されている。1
0.10aは前記バッキングプレートlの下方側に別途
設けられた冷却装置を示す。
5.5a is for each yoke 3 to cover the yoke 3.3a.
.. 3a shows the ground shield plate provided on the outside,
The shield plate 5.5a is grounded while being insulated from the yoke 3.3a, the backing plate Ia, etc. 1
0.10a indicates a cooling device separately provided below the backing plate l.

本実施例は以上の構成からなり、次にその使用法並びに
作用について説明する。  。
The present embodiment has the above configuration, and its usage and operation will be explained next. .

先ず、前記装置の周辺雰囲気をアルゴン等のスパッタガ
スの低圧雰囲気状態とした後に、両ターゲット4.4a
を陰極とすべく電圧v7を印加させることにより、両タ
ーゲット4.4aをスパッタせしめれば、両ターゲット
4.48間の磁界空間部7内では該ターゲット4.4a
の金属原子、二次電子、及びアルゴンガスイオン等が飛
散したプラズマ状態が発生する。
First, after setting the surrounding atmosphere of the apparatus to a low pressure atmosphere of sputtering gas such as argon, both targets 4.4a
If both targets 4.4a are sputtered by applying a voltage v7 to serve as a cathode, the target 4.4a will be sputtered in the magnetic field space 7 between both targets 4.48.
A plasma state is generated in which metal atoms, secondary electrons, argon gas ions, etc. are scattered.

従って、前記プラズマ空間内のスパッタ放出されたター
ゲット金属原子は空間部7の上方に設けられた基板13
の表面に到達して均一状態に付着することとなって所定
の薄膜形成が行える。また、その際空間部7内に発生さ
れたプラズマ空間内のターゲット金属原子等の一部は中
間電極6の表面側に衝突して付着、堆積する現象を生じ
る。
Therefore, the sputtered target metal atoms in the plasma space are transferred to the substrate 13 provided above the space 7.
It reaches the surface and adheres uniformly to form a predetermined thin film. Further, at this time, a part of the target metal atoms and the like in the plasma space generated in the space 7 collide with the surface side of the intermediate electrode 6, causing a phenomenon in which they adhere and deposit.

一方、中間電極6には予め両ターゲッ)4.4aよりも
低電圧の負の電圧v1を印加させて陰極としておく。す
なわち、例えばVt=600ボルト、vt=350ボル
ト、の如(設定する。従って、前記中間電極6の表面部
に於いてもマグネトロン放電が生じるために、該中間電
極6の表面に付着されたスパッタ粒子が前記マグネトロ
ン放電によって再スパツタされて空間部7側に再度放出
されるのである。すなわち、中間電極6の表面部に於い
てはターゲット4.4aの金属原子等の付着現象を生じ
ると共に、該付着された金属原子等が再度スパッタされ
て空間部7内に放出されることを繰り返し行い、これに
よって基板13での薄膜生成速度が高速となるのである
On the other hand, a negative voltage v1 lower than both targets 4.4a is applied in advance to the intermediate electrode 6 to serve as a cathode. That is, for example, Vt = 600 volts, vt = 350 volts (set). Therefore, since magnetron discharge occurs also on the surface of the intermediate electrode 6, the spatter attached to the surface of the intermediate electrode 6 is The particles are sputtered again by the magnetron discharge and ejected again toward the space 7. That is, the metal atoms of the target 4.4a adhere to the surface of the intermediate electrode 6, and The attached metal atoms and the like are repeatedly sputtered and released into the space 7, thereby increasing the rate of thin film formation on the substrate 13.

而して、前記中間電極6はターゲット4.4aのスパッ
タ面12.12aに於けるスパッタよりも抑制された状
態なるために、該中間電極6へのスパッタ粒子の付着速
度の方が、スパッタによる浸食速度よりも高速となって
、中間電極6自体がスパッタされる様なことは好適に回
避される。よって、該中間電極6の材料成分が基板13
に生成される薄膜内に含有される様なことはない。
Since the intermediate electrode 6 is in a state in which sputtering is suppressed more than the sputtering on the sputtering surface 12.12a of the target 4.4a, the adhesion speed of sputtered particles to the intermediate electrode 6 is higher than that due to sputtering. A situation in which the intermediate electrode 6 itself is sputtered due to a speed higher than the erosion rate is preferably avoided. Therefore, the material component of the intermediate electrode 6 is the same as that of the substrate 13.
There is no possibility that it will be contained in the thin film produced.

また、中間電極6から放出される二次電子はE×Bドリ
フトで中間電極上を移動しながらスパッタガスのイオン
化を促進させる作用、即ちマグネトロン放電を生じるこ
ととなって、空間部7内のプラズマ密度が一層高くなり
、薄膜生成速度の高速化が一層図れることとなる。
In addition, the secondary electrons emitted from the intermediate electrode 6 move on the intermediate electrode due to EXB drift and promote the ionization of the sputtering gas, that is, generate a magnetron discharge, causing plasma in the space 7. The density is further increased, and the thin film production rate can be further increased.

尚、上記実施例に於いては、ターゲット4.4a及び中
間電極6の各印加電圧値を、夫々600vと350vに
設定した例を挙げたが、本発明に係る各印加電圧値は必
ずしも上記の如く限定されるものではない。本件出願人
の実験によれば、材質が純鉄のターゲットの場合に、タ
ーゲット印加電圧を500■、中間電極への印加電圧を
350Vとした場合に中間電極6の表面に鉄の僅かな堆
積が認められ、本発明の意図する作用、効果が生じたこ
とが確認できた。また他の設定値での実験では、中間電
極への印加電圧をターゲット印加電圧よりも概ね150
〜250■程度低い値とした場合に良好な結果が得られ
たが、これらの値はターゲットの材質やスパッタガス雰
囲気等によってかなり左右されることが確認された。従
って、本発明はその具体的な数値は問うものではない。
In the above embodiment, the applied voltage values of the target 4.4a and the intermediate electrode 6 were set to 600v and 350v, respectively, but the applied voltage values according to the present invention are not necessarily the same as those described above. However, it is not limited to this. According to the applicant's experiments, in the case of a target made of pure iron, a slight amount of iron was deposited on the surface of the intermediate electrode 6 when the voltage applied to the target was 500 V and the voltage applied to the intermediate electrode was 350 V. It was confirmed that the intended effects and effects of the present invention were achieved. In addition, in experiments using other setting values, the voltage applied to the intermediate electrode was approximately 150° lower than the target applied voltage.
Although good results were obtained when the value was as low as ~250 .mu., it was confirmed that these values were considerably influenced by the material of the target, the sputtering gas atmosphere, etc. Therefore, the present invention does not require specific numerical values.

要は、中間電極6はターゲット4.4aの背面側で且つ
磁界空間部7と対面する位置に設けられて、空間部7に
発生される空間プラズマのスパッタ粒子が該中間電極6
に付着する速度よりも低速のスパッタが行われるべく前
記両ターゲット4.4aよりも低電圧の陰極として構成
されておればよい。
In short, the intermediate electrode 6 is provided on the back side of the target 4.4a and at a position facing the magnetic field space 7, so that the sputtered particles of the spatial plasma generated in the space 7 are transferred to the intermediate electrode 6.
It is sufficient that the cathode is configured with a voltage lower than that of both targets 4.4a so that sputtering can be performed at a speed lower than that of the targets 4.4a.

よって、該中間電極6の具体的な取付手段も決して上記
実施例の如く限定されるものではない。
Therefore, the specific means for attaching the intermediate electrode 6 is by no means limited to the above embodiments.

また、両ターゲット及び中間電極の電圧印加に際して上
記実施例の如く一個の電源を併用すれば装置の構成簡略
化が図れる利点が得られるが、本発明は当然ながらター
ゲットと中間電極とを別個の電源で印加してもよい。
Furthermore, when applying voltages to both targets and the intermediate electrode, it is possible to simplify the configuration of the apparatus by using a single power supply as in the above embodiment, but the present invention naturally provides the advantage that the target and the intermediate electrode are connected to separate power supplies. It may be applied by

更に、本発明はその他の各部の具体的な構成も決して上
記実施例の如く限定されず、これらは全て本発明の意図
する範囲内で設計変更自在である。
Further, the present invention is by no means limited to the specific configurations of other parts as in the above embodiments, and all of these can be freely modified within the intended scope of the present invention.

すなわち、空間部7に磁界を発生させるための磁石の配
置は従来例としての第3図の如き配置でもよいことは勿
論のこと、両ターゲット4.4aの形状は円形リング状
に限らず、例えば第2図に示す如く長方形状のリング状
にしてもよい。但し、この場合には中間電極6の形状も
これに応じて変更せねばならないことは言う迄もない。
That is, it goes without saying that the arrangement of the magnets for generating a magnetic field in the space 7 may be as shown in the conventional arrangement shown in FIG. It may be formed into a rectangular ring shape as shown in FIG. However, in this case, it goes without saying that the shape of the intermediate electrode 6 must also be changed accordingly.

その他、内側ターゲット4の内側に位置する内側ヨーク
3は本発明の必須要件ではないが、該内側ヨーク3がタ
ーゲット4と同材質であれば、その上方のグランドシー
ルド板5を除去しても実用上は何ら支障ない。
In addition, the inner yoke 3 located inside the inner target 4 is not an essential requirement of the present invention, but if the inner yoke 3 is made of the same material as the target 4, it is practical even if the ground shield plate 5 above it is removed. There is no problem above.

(発明の効果) 叙上の様に、本発明は内側ターゲットと外側ターゲット
との両スパッタ面間に形成された磁界空間部に対面させ
て設けた中間電極を両ターゲットよりも低電圧の陰極と
して、空間部から中間電極の表面部に付着されるターゲ
ット原子等のスパッタ粒子をその付着速度よりも低速で
再スパツタさせる様に構成してなるために、該中間電極
のスパッタによって中間電極自体の成分が空間部側に放
出される様なことを適切に防止できて、生成薄膜の品質
を高品質に保つことができることは勿論のこと、中間電
極側には従来のアノードを用いた手段の如くターゲット
原子等が一方的に付着堆積する様な無駄を生じることな
く、中間電極に付着されたターゲット原子等を再度のス
パッタによって薄膜生成に利用できることとなり、その
結果所定の薄膜生成速度が従来に比してかなり高速で効
率良く行えるという格別な効果を得るに至った。
(Effects of the Invention) As described above, the present invention uses the intermediate electrode provided facing the magnetic field space formed between the sputtering surfaces of the inner target and the outer target as a cathode with a lower voltage than both targets. Since the structure is configured so that sputtered particles such as target atoms that are attached to the surface of the intermediate electrode from the space are re-sputtered at a speed lower than the deposition speed, the components of the intermediate electrode itself are sputtered by the sputtering of the intermediate electrode. It goes without saying that it is possible to appropriately prevent the release of gas into the space side, and maintain the quality of the produced thin film at a high level. The target atoms, etc. attached to the intermediate electrode can be used for thin film production by sputtering again, without causing waste such as unilateral adhesion and deposition of atoms, etc., and as a result, the predetermined thin film production speed can be increased compared to the conventional method. We have achieved the extraordinary effect of being able to perform this process fairly quickly and efficiently.

しかも、本発明は前記中間電極側のスパッタによって放
出される二次電子により磁界空間部内のプラズマ密度を
一層高めることができて、より低ガス圧、低電圧の条件
下でのスパッタが可能となり、また薄膜生成作業の効率
を一層向上させることができるという効果をも有するに
至った。
Moreover, the present invention can further increase the plasma density in the magnetic field space by the secondary electrons emitted by the sputtering on the intermediate electrode side, making it possible to perform sputtering under conditions of lower gas pressure and lower voltage. Furthermore, the present invention has the effect that the efficiency of thin film production work can be further improved.

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

第1図は本発明に係るスパッタ装置の一実施例を示す概
略正面断面図。 第2図は他の実施例を示す概略平面図。 第3図及び第4図は従来例を示し、第3図(イ)は要部
概略正面断面図、第3図(ロ)は概略平面図、第4図は
要部概略正面断面図。 4・・・内側ターゲット    4a・・・外側ターゲ
ット6・・・中間電極       7・・・磁界空間
部12.12a・・・スパッタ面 出願人 株式会社大阪真空機器製作所 代理人  弁理士  藤 本  昇 第11!1 第3i!1 (イ) (ロ)
FIG. 1 is a schematic front sectional view showing an embodiment of a sputtering apparatus according to the present invention. FIG. 2 is a schematic plan view showing another embodiment. 3 and 4 show a conventional example, in which FIG. 3(A) is a schematic front sectional view of the main part, FIG. 3(B) is a schematic plan view, and FIG. 4 is a schematic front sectional view of the main part. 4...Inner target 4a...Outer target 6...Intermediate electrode 7...Magnetic field space 12.12a...Sputtering surface Applicant Osaka Vacuum Equipment Manufacturing Co., Ltd. Agent Patent attorney Noboru Fujimoto No. 11 !1 3rd i! 1 (a) (b)

Claims (1)

【特許請求の範囲】[Claims] 外周側面をスパッタ面12とする内側ターゲット4の外
方周囲に、前記スパッタ面12と対面した内周面をスパ
ッタ面12aとするリング状の外側ターゲット4aが配
置されて、該両ターゲット4、4aのスパッタ面12、
12a間には両ターゲット4、4aのスパッタ時に空間
プラズマが発生される磁界空間部7が形成されてなるス
パッタ装置であって、前記ターゲット4、4aの背面側
で前記空間部7と対面する位置には中間電極6が設けら
れ、且つ該中間電極6は、空間部7に発生される空間プ
ラズマのスパッタ粒子が該中間電極6に付着する速度よ
りも低速のスパッタ浸食が行われるべく前記両ターゲッ
ト4、4aよりも低電圧の陰極として構成されてなるこ
とを特徴とするスパッタ装置。
A ring-shaped outer target 4a whose inner peripheral surface facing the sputtering surface 12 is a sputtering surface 12a is disposed around the outer circumference of the inner target 4 whose outer peripheral side surface is a sputtering surface 12, and both targets 4, 4a sputtering surface 12,
This is a sputtering apparatus in which a magnetic field space 7 is formed between the targets 4 and 12a in which spatial plasma is generated during sputtering of both targets 4 and 4a, and a position facing the space 7 on the back side of the targets 4 and 4a. is provided with an intermediate electrode 6, and the intermediate electrode 6 is connected to both targets so that sputter erosion is performed at a speed lower than the rate at which sputter particles of the spatial plasma generated in the space 7 adhere to the intermediate electrode 6. 4. A sputtering apparatus characterized in that the sputtering apparatus is configured as a cathode with a lower voltage than those of 4 and 4a.
JP62052706A 1987-03-06 1987-03-06 Spatter equipment Expired - Fee Related JP2580149B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62052706A JP2580149B2 (en) 1987-03-06 1987-03-06 Spatter equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62052706A JP2580149B2 (en) 1987-03-06 1987-03-06 Spatter equipment

Publications (2)

Publication Number Publication Date
JPS63219579A true JPS63219579A (en) 1988-09-13
JP2580149B2 JP2580149B2 (en) 1997-02-12

Family

ID=12922337

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62052706A Expired - Fee Related JP2580149B2 (en) 1987-03-06 1987-03-06 Spatter equipment

Country Status (1)

Country Link
JP (1) JP2580149B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6623607B1 (en) * 1997-11-20 2003-09-23 Balzers Hochvakuum Ag Substrate coated with an MGO-layer
WO2011062943A3 (en) * 2009-11-18 2011-09-15 Applied Materials, Inc. Planar magnetron sputtering source producing high target utilization and stable coating uniformity over lifetime

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6623607B1 (en) * 1997-11-20 2003-09-23 Balzers Hochvakuum Ag Substrate coated with an MGO-layer
WO2011062943A3 (en) * 2009-11-18 2011-09-15 Applied Materials, Inc. Planar magnetron sputtering source producing high target utilization and stable coating uniformity over lifetime

Also Published As

Publication number Publication date
JP2580149B2 (en) 1997-02-12

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