JPS62127465A - Sputtering device - Google Patents
Sputtering deviceInfo
- Publication number
- JPS62127465A JPS62127465A JP26768185A JP26768185A JPS62127465A JP S62127465 A JPS62127465 A JP S62127465A JP 26768185 A JP26768185 A JP 26768185A JP 26768185 A JP26768185 A JP 26768185A JP S62127465 A JPS62127465 A JP S62127465A
- Authority
- JP
- Japan
- Prior art keywords
- substrate
- magnets
- target
- magnet
- auxiliary
- 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
Links
Landscapes
- Electrodes Of Semiconductors (AREA)
- Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)
- Physical Vapour Deposition (AREA)
Abstract
Description
【発明の詳細な説明】
〔(既要〕
スパッタ装置において、プラズマ閉じ込め磁石と略同様
な磁石を対向設置することにより、プラズマ閉じ込め磁
石の磁力線が被加工物たる基板をよぎらないようにする
ことによって、磁力線に沿ってスパイラル運動しながら
基板に突入し基板温度を上げる電子をなくする。[Detailed Description of the Invention] [(Already required)] To prevent the lines of magnetic force of the plasma confinement magnet from crossing a substrate, which is a workpiece, by arranging a magnet substantially similar to the plasma confinement magnet to face each other in a sputtering apparatus. This eliminates electrons that move spirally along the lines of magnetic force and rush into the substrate, raising the temperature of the substrate.
本発明は半導体基板等にAI被被膜の被着を行うマグネ
トロン型スパッタ装置の構造に関する。The present invention relates to the structure of a magnetron sputtering apparatus for depositing an AI coating onto a semiconductor substrate or the like.
スパッタ装置は低圧気体放電を利用して薄膜を形成する
ものであるが、近時マグネトロン型のものを使用するよ
うになって膜成長速度が上がり広く実用化されている。Sputtering devices form thin films using low-pressure gas discharge, and recently magnetron-type devices have been used to increase the film growth rate and are now widely put into practical use.
マグネトロン型スパッタ装置はターゲットの形状からプ
レーナマグネトロン型、リングマグネトロン型、同軸マ
グネトロン型と分類されている。Magnetron sputtering devices are classified into planar magnetron types, ring magnetron types, and coaxial magnetron types based on the shape of the target.
いづれの形式のマグネトロン型スパッタ装置も、真空容
器内に計等のガスを導入してDCまたはRF等でグロー
放電させて、ガスをプラズマ化し、カソードのターゲッ
ト材料をスパッタしてターゲットに対置した基板上に堆
積する際、ターゲ7)の裏面に装着された永久磁石によ
る磁界でプラズマ中の電子を閉じ込めArイオンの発生
を増進し、プラズマ密度を上げスパッタ効率を向上する
ものである。In both types of magnetron type sputtering equipment, a gas such as a gas is introduced into a vacuum chamber and a glow discharge is performed using DC or RF to turn the gas into plasma, and the target material for the cathode is sputtered onto a substrate placed opposite to the target. When depositing on the target 7), electrons in the plasma are confined by a magnetic field generated by a permanent magnet attached to the back surface of the target 7), thereby promoting the generation of Ar ions, increasing the plasma density and improving the sputtering efficiency.
そのためスパッタされたターゲット材料は対向配置され
た基板に効率よく到達し、高速で被膜が形成される。Therefore, the sputtered target material efficiently reaches the opposing substrate, and a film is formed at high speed.
しかし、基板の一方向にのみプラズマ閉じ込め磁石をも
った形式のマグネトロン型スパッタ装置では、基板と同
電位のアノードを設けたり基板とターゲット距離を変化
させても、基板を貫く磁力線を完全に零には出来ない。However, with magnetron sputtering equipment that has a plasma confinement magnet only in one direction of the substrate, even if an anode with the same potential as the substrate is installed or the distance between the substrate and the target is changed, the lines of magnetic force penetrating the substrate can be completely reduced to zero. I can't.
このためその貫入磁力線に巻きついてスパイラル状に飛
来する電子が基板に衝突し、基板の温度上昇を起こし堆
積膜の膜質が局部的に麹化する。温度差異はAI被被膜
場合はグレインサイズ差異となり、膜の光沢の変化とな
って現れる。グレインサイズ変化はエツチング、マイグ
レーションに好ましくないので改善が望まれている。For this reason, electrons that fly around in a spiral manner around the penetrating magnetic field line collide with the substrate, raising the temperature of the substrate and causing the quality of the deposited film to become malt locally. In the case of an AI coating, the temperature difference results in a grain size difference, which manifests as a change in the gloss of the film. Changes in grain size are unfavorable for etching and migration, so improvement is desired.
第2図は従来例によるプレーナマグネトロン型スパッタ
装置を模式的に示す断面図である。FIG. 2 is a sectional view schematically showing a conventional planar magnetron type sputtering apparatus.
図において、lは平面状のAIのターゲットで負電圧を
印加する。このターゲット1の裏面に接して永久磁石で
出来たプラズマ閉じ込め磁石2a、2bの磁極がある。In the figure, l is a planar AI target to which a negative voltage is applied. In contact with the back surface of this target 1 are the magnetic poles of plasma confinement magnets 2a and 2b made of permanent magnets.
プラズマ閉じ込め磁石2aは円柱状磁石のN極、プラズ
マ閉じ込め磁石2bは中空円筒状のS極となっている。The plasma confinement magnet 2a is a cylindrical north pole, and the plasma confinement magnet 2b is a hollow cylindrical south pole.
ターゲット1の上方の、このターゲット1に対向した位
置に半導体基板3を置き接地する。A semiconductor substrate 3 is placed above the target 1 at a position facing the target 1 and grounded.
ターゲット1の表面上方にはプラズマ閉じ込め磁石2a
、2bによる磁界を生じ、その磁力線がN極よりS極に
向かう。4aは基板3にあたることなくN極よりS極に
向かう磁力線、4bは基板3をよぎる貫入磁力線である
。Above the surface of the target 1 is a plasma confinement magnet 2a.
, 2b, and the lines of magnetic force are directed from the north pole to the south pole. 4a is a line of magnetic force that goes from the north pole to the south pole without hitting the substrate 3, and 4b is a line of magnetic force that crosses the substrate 3.
殆ど大部分の電子は放射状に閉じた磁力線4aによりタ
ーゲット1近傍に閉じ込められ、トロイダル運動をしな
からArイオンの発生を増進する。Most of the electrons are confined in the vicinity of the target 1 by the radially closed magnetic lines of force 4a, and do not perform toroidal motion, thereby promoting the generation of Ar ions.
計イオンが高い電流密度で衝撃するのでスパッタによる
基板3におけるAI膜の生成速度は高速化される。また
プラズマをターゲット1の近傍の局所的空間に閉じ込め
ているので基板3の温度上昇も非常に少ない。Since the ions are bombarded with a high current density, the rate at which the AI film is formed on the substrate 3 by sputtering is increased. Furthermore, since the plasma is confined in a local space near the target 1, the temperature rise of the substrate 3 is also very small.
しかしながら、貫入磁力&i4bの如く基板3に貫入す
る磁力線があり、ターゲット1から基板3を離すと貫入
磁力線4bの数は減少するが完全に零となることはない
。However, there are magnetic lines of force penetrating the substrate 3, such as the penetrating magnetic force &i4b, and when the substrate 3 is separated from the target 1, the number of penetrating lines of magnetic force 4b decreases, but does not become completely zero.
従来のマグネトロン型スパッタ装置に於ては、基板を横
切る磁力線があり、これの影響下に入った電子はスパイ
ラル運動をしながら基板に衝突し基板の温度を局所的に
上げる。局所的温度上昇は被着Al膜の膜質むら(主と
してグレインサイズのむら)となり、これがひいてはエ
ツチングや、マイグレーションに悪い結果を招く要因と
なっている。In a conventional magnetron type sputtering apparatus, there are magnetic lines of force that cross the substrate, and electrons that come under the influence of these lines collide with the substrate while moving in a spiral manner, thereby locally increasing the temperature of the substrate. A local temperature rise causes unevenness in the quality of the deposited Al film (mainly unevenness in grain size), which in turn causes bad results in etching and migration.
上記問題点の解決は、ターゲット表面近傍に閉磁界を形
成する磁石を備えたスパッタ装置において、前記磁石の
形成する磁力線分布と同じような磁力線分布を形成する
補助磁石を前記磁石の対向位置に設置し、且つターゲッ
ト材料を被着する基板はターゲットと補助磁石の中間領
域の磁気的中立面またはそれより補助磁石寄りに設置す
ることが出来るようにした本発明によるスパッタ装置に
より達成される。The solution to the above problem is to install an auxiliary magnet that forms a magnetic field line distribution similar to that formed by the magnet in a sputtering apparatus equipped with a magnet that forms a closed magnetic field near the target surface, at a position opposite to the magnet. This is achieved by the sputtering apparatus according to the present invention in which the substrate to which the target material is deposited can be placed on the magnetic neutral plane in the intermediate region between the target and the auxiliary magnet or closer to the auxiliary magnet.
本発明はプラズマ閉じ込め磁石と同様な磁力線分布を持
つ補助磁石を向い合わせに対置し、プラズマ閉じ込め磁
石からの磁力線のターゲット上方への伸びを限定し、こ
のプラズマ閉じ込め磁石による磁界外に基板を置くこと
により、プラズマ閉じ込め磁石による磁力線で基板に貫
入するものを皆無とするものである。斯くすることによ
り、磁力線に巻きついて飛来する電子を完全になくし基
板の局所的温度上昇をなくする。In the present invention, auxiliary magnets having the same magnetic field line distribution as the plasma confinement magnet are placed opposite each other to limit the extension of the magnetic field lines from the plasma confinement magnet above the target, and the substrate is placed outside the magnetic field of the plasma confinement magnet. This eliminates any penetration of the substrate by magnetic lines of force caused by the plasma confinement magnet. By doing so, the electrons that fly around the magnetic lines of force are completely eliminated, and the local temperature rise of the substrate is eliminated.
第1図は本発明による補助磁石付プレーナマグネトロン
型スパッタ装置を模式的に示す断面図である。FIG. 1 is a sectional view schematically showing a planar magnetron type sputtering apparatus with an auxiliary magnet according to the present invention.
図において、第2図と同じ名称のものは同じ記号で示す
。In the figure, parts with the same names as in FIG. 2 are indicated by the same symbols.
図において、1は平面状のAIのターゲットで、負電圧
を印加する。In the figure, 1 is a planar AI target to which a negative voltage is applied.
このターゲット1の裏面に接して永久磁石で出来たプラ
ズマ閉じ込め磁石2a、2bの磁極をもつ。プラズマ閉
じ込め磁石2aは円柱状磁石のN極、プラズマ閉じ込め
磁石2bは中空円筒状のS極となっている。In contact with the back surface of this target 1, there are magnetic poles of plasma confinement magnets 2a and 2b made of permanent magnets. The plasma confinement magnet 2a is a cylindrical north pole, and the plasma confinement magnet 2b is a hollow cylindrical south pole.
プラズマ閉じ込め磁石2a、2bと同じ構造の補助磁石
5a、5bを、プラズマ閉じ込め磁石2a、2bと向い
合わせに設置する。この補助磁石5a、5b下面にはタ
ーゲット1と同じ形状のAIの補助板6を設け、これに
は電位はかけない。Auxiliary magnets 5a, 5b having the same structure as the plasma confinement magnets 2a, 2b are installed to face the plasma confinement magnets 2a, 2b. An AI auxiliary plate 6 having the same shape as the target 1 is provided on the lower surface of the auxiliary magnets 5a and 5b, and no potential is applied to this plate.
かくするときはプラズマ閉じ込め磁石2a、2bが形成
する磁力線分布と同じものを補助磁石5a、5bによっ
て鏡像的に上方に、磁力線8aとして示す如く形成する
ことが出来る。 しかるときは両磁石の中間高さに磁界
のない磁気的中立面7を形成することが出来る。 基板
3はこの磁気的中立面7又はそれよりやや補助磁石5a
、5b寄りに設置し、かつ接地する。 このようにする
ときは、下のプラズマ閉じ込め磁石2a、2bにより形
成される磁力線で基板3を貫くものは全くなく、従って
貫入磁力線の作用で基板3に衝突する電子もなくなり、
基板3の温度も局所的に上がることがなくなる。In this case, the same magnetic field line distribution as that formed by the plasma confinement magnets 2a and 2b can be formed upward in a mirror image manner by the auxiliary magnets 5a and 5b as shown as magnetic field lines 8a. In such a case, a magnetic neutral plane 7 without a magnetic field can be formed at a height midway between both magnets. The substrate 3 is located at this magnetic neutral plane 7 or slightly more than the auxiliary magnet 5a.
, installed near 5b and grounded. When doing this, there are no magnetic lines of force formed by the lower plasma confinement magnets 2a and 2b that penetrate the substrate 3, and therefore no electrons collide with the substrate 3 due to the action of the penetrating lines of magnetic force.
The temperature of the substrate 3 will also no longer rise locally.
ターゲットはAIとして説明したが、A1合金、高融点
金属またはそのシリサイドであってもよい。Although the target has been described as being AI, it may also be an Al alloy, a high melting point metal, or a silicide thereof.
この補助磁石5a、5bと補助板6の位置は真空系内外
いづれであってもよい。The auxiliary magnets 5a, 5b and the auxiliary plate 6 may be located either inside or outside the vacuum system.
又、補助磁石5a、5bはプラズマ閉じ込め磁石2a、
2bと大略同じ磁力線分布形状を形成するものであれば
、若干強度が異なってもよい。Further, the auxiliary magnets 5a and 5b are plasma confinement magnets 2a,
As long as it forms approximately the same magnetic force line distribution shape as 2b, the strength may be slightly different.
又、磁気的中立面はプレーナ型に限らず他の形式のマグ
ネトロン型スパッタ装置にも形成可能である。Further, the magnetic neutral plane can be formed not only in the planar type but also in other types of magnetron type sputtering equipment.
以上詳細に説明したように本発明によるスパッタ装置に
よれば、基板に衝撃を与える電子がなくなり、基板の局
所的温度上昇がなく、均質なグレインサイズの被膜を形
成することが出来、エツチングむら、マイグレーション
等を防止出来る。As explained in detail above, according to the sputtering apparatus according to the present invention, there are no electrons impacting the substrate, there is no local temperature rise of the substrate, a film with a uniform grain size can be formed, and etching unevenness can be avoided. Migration etc. can be prevented.
第1図は本発明による補助磁石付マグネトロン型スパッ
タ装置の断面図である。
第2図は従来例によるマグネトロン型スパッタ装置の断
面図である。
図において、
1はターゲット、
2a、2bはプラズマ閉じ込め磁石、
3は基板、
4aは磁力線、
5a、5bは補助磁石、
6は補助板、
7は磁気的中立面、
8aは磁力線
プラズマ1hし途ジM漠乃FIG. 1 is a sectional view of a magnetron type sputtering apparatus with an auxiliary magnet according to the present invention. FIG. 2 is a sectional view of a conventional magnetron type sputtering apparatus. In the figure, 1 is a target, 2a and 2b are plasma confinement magnets, 3 is a substrate, 4a is a magnetic field line, 5a and 5b are auxiliary magnets, 6 is an auxiliary plate, 7 is a magnetic neutral plane, 8a is a magnetic field line plasma 1h Ji M Kuano
Claims (1)
パッタ装置において、前記磁石の形成する磁力線分布と
同じような磁力線分布を形成する補助磁石を前記磁石の
対向位置に設置し、且つターゲット材料を被着する基板
はターゲットと補助磁石の中間領域の磁気的中立面また
はそれより補助磁石寄りに設置することが出来るように
したことを特徴とするスパッタ装置。In a sputtering apparatus equipped with a magnet that forms a closed magnetic field near the target surface, an auxiliary magnet that forms a magnetic field line distribution similar to the magnetic field line distribution formed by the magnet is installed at a position opposite to the magnet, and the target material is covered with the target material. A sputtering apparatus characterized in that a substrate to be deposited can be placed on a magnetic neutral plane in an intermediate region between a target and an auxiliary magnet or closer to the auxiliary magnet.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26768185A JPS62127465A (en) | 1985-11-28 | 1985-11-28 | Sputtering device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26768185A JPS62127465A (en) | 1985-11-28 | 1985-11-28 | Sputtering device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62127465A true JPS62127465A (en) | 1987-06-09 |
Family
ID=17448049
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP26768185A Pending JPS62127465A (en) | 1985-11-28 | 1985-11-28 | Sputtering device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62127465A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01309966A (en) * | 1988-06-08 | 1989-12-14 | Matsushita Electric Ind Co Ltd | Sputtering device |
EP1892317A1 (en) * | 2006-08-24 | 2008-02-27 | Applied Materials GmbH & Co. KG | Method and apparatus for sputtering . |
-
1985
- 1985-11-28 JP JP26768185A patent/JPS62127465A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01309966A (en) * | 1988-06-08 | 1989-12-14 | Matsushita Electric Ind Co Ltd | Sputtering device |
EP1892317A1 (en) * | 2006-08-24 | 2008-02-27 | Applied Materials GmbH & Co. KG | Method and apparatus for sputtering . |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
KR100396456B1 (en) | High target utilization magnetic arrangement for a truncated conical sputtering target | |
US6254745B1 (en) | Ionized physical vapor deposition method and apparatus with magnetic bucket and concentric plasma and material source | |
AU746645C (en) | Method and apparatus for deposition of biaxially textured coatings | |
US4710283A (en) | Cold cathode ion beam source | |
KR100212087B1 (en) | Sputtering apparatus | |
JPH1171670A (en) | Sputtering device | |
US6683425B1 (en) | Null-field magnetron apparatus with essentially flat target | |
US6066242A (en) | Conical sputtering target | |
JPS6116347B2 (en) | ||
EP1144713B1 (en) | High target utilization magnetic arrangement for a truncated conical sputtering target | |
JPH079062B2 (en) | Spatter device | |
Spencer et al. | The design and performance of planar magnetron sputtering cathodes | |
US20020195336A1 (en) | System for unbalanced magnetron sputtering with AC power | |
JPS63317671A (en) | Method and device for sputtering | |
JPS62127465A (en) | Sputtering device | |
JPS6128029B2 (en) | ||
JPH0692632B2 (en) | Flat plate magnetron sputtering system | |
JPH0525625A (en) | Magnetron sputtering cathode | |
JP2902822B2 (en) | Planar magnetron sputter electrode | |
JPS6176673A (en) | Sputtering method | |
RU2242821C2 (en) | Magnetron spraying system | |
US6432286B1 (en) | Conical sputtering target | |
US6235170B1 (en) | Conical sputtering target | |
JP2769572B2 (en) | Cathode for magnetron sputtering | |
JPS6233764A (en) | Sputtering device |