JPH01108375A - Magnetron sputtering device - Google Patents

Magnetron sputtering device

Info

Publication number
JPH01108375A
JPH01108375A JP26365587A JP26365587A JPH01108375A JP H01108375 A JPH01108375 A JP H01108375A JP 26365587 A JP26365587 A JP 26365587A JP 26365587 A JP26365587 A JP 26365587A JP H01108375 A JPH01108375 A JP H01108375A
Authority
JP
Japan
Prior art keywords
magnet
target
magnetic field
magnetic circuit
annular magnet
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
JP26365587A
Other languages
Japanese (ja)
Other versions
JPH0826454B2 (en
Inventor
Hitoshi Sato
均 佐藤
Hideaki Sato
英明 佐藤
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.)
Mitsubishi Steel Mfg Co Ltd
Original Assignee
Mitsubishi Steel Mfg Co 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 Mitsubishi Steel Mfg Co Ltd filed Critical Mitsubishi Steel Mfg Co Ltd
Priority to JP62263655A priority Critical patent/JPH0826454B2/en
Publication of JPH01108375A publication Critical patent/JPH01108375A/en
Publication of JPH0826454B2 publication Critical patent/JPH0826454B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To reduce the unused region of a target and to increase the film forming rate of the title device by forming a magnetic field generating magnetic circuit with a central magnet, an annular magnet, and an annular magnet having a magnetization direction parallel to the target surface from the center toward the outer periphery. CONSTITUTION:The central magnet 11 having a magnetization direction vertical to the target surface is arranged at the center of a magnetic circuit, and the annular magnet 12 having a magnetization direction reverse to that of the central magnet 11 is arranged on the outer periphery. Furthermore, the annular magnet 13 having a magnetization direction parallel to the target surface and extending from the outer periphery to the center is arranged to bridge the upper and lower parts of the central magnet 11 and the annular magnet 12. The ferromagnetic field region is increased by about 1.3-1.8 times as compared with the conventional device, hence the erosion region to be sputtered is increased, and the utilization efficiency of the target is improved.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、ターゲット支持台に内蔵する永久磁石磁気回
路により、大きな強磁界領域を発生させ、広いスパッタ
領域を得るマグネトロンスパッタ装置に関するものであ
る。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a magnetron sputtering device that generates a large strong magnetic field region using a permanent magnet magnetic circuit built into a target support base and obtains a wide sputtering region. .

[従来の技術] マグネトロンスパッタ装置は、第8図に示すように、ス
パッタガス導入管2および排気装置3を備えた真空容器
1内に、ターゲット4および磁気回路を内蔵したターゲ
ット支持台5と、これに対抗して薄膜を形成すべき基板
6が基板ホルダー7によって保持されている。
[Prior Art] As shown in FIG. 8, a magnetron sputtering apparatus includes a target support 5 containing a target 4 and a magnetic circuit in a vacuum vessel 1 equipped with a sputtering gas introduction pipe 2 and an exhaust device 3; In contrast, a substrate 6 on which a thin film is to be formed is held by a substrate holder 7.

このようなマグネトロンスパッタ装置を用いて基板6表
面に薄膜を形成するには、真空容器1内を排気装置3に
より真空排気した後、アルゴンガスなどのスパッタガス
をスパッタガス導入管7より導入した後、ターゲット4
に所定電圧を印加する。このとき発生したスパッタガス
プラズマはターゲット支持台5に内蔵された環状磁石と
中央磁石よりなる磁気回路の発生する磁界に集束されて
、ターゲット4に衝突することにより、その表面のスパ
ッタ物質がスバッタされて基板6上に大きな堆積速度で
[1を生成する。
In order to form a thin film on the surface of the substrate 6 using such a magnetron sputtering device, the inside of the vacuum chamber 1 is evacuated by the exhaust device 3, and then a sputter gas such as argon gas is introduced from the sputter gas introduction pipe 7. , target 4
Apply a predetermined voltage to. The sputtering gas plasma generated at this time is focused by a magnetic field generated by a magnetic circuit consisting of an annular magnet and a central magnet built into the target support 5, and collides with the target 4, thereby sputtering the sputtered material on the surface. [1] is produced on the substrate 6 at a high deposition rate.

[発明が解決しようとする問題点] 上記のようなマグネトロンスパッタ装置においては、タ
ーゲット支持台に内蔵した磁石により発生する磁界のタ
ーゲット中央から外側もしくは外側から内側に向い、タ
ーゲット表面と平行な成分(以下B1とする)によって
、ガスプラズマが集束されてスパッタされることから、
ターゲット上の環状強磁界!i域にガスプラズマが集り
、この領域が局所的にスパッタされて、浸食された環状
エロージョン領域となり、その他の領域はほとんどスパ
ッタされない領域である。
[Problems to be Solved by the Invention] In the magnetron sputtering apparatus as described above, the component of the magnetic field generated by the magnet built in the target support is directed outward from the center of the target or from the outside to the inside, and is parallel to the target surface ( Since the gas plasma is focused and sputtered by B1),
Annular strong magnetic field on the target! The gas plasma gathers in the i region, and this region is locally sputtered to become an eroded annular erosion region, and the other regions are hardly sputtered.

ここで強磁界領域とは、ターゲット表面でBRがその最
大値の80%以上の磁界強度を示す領域のことである。
Here, the strong magnetic field region refers to a region where BR exhibits a magnetic field strength of 80% or more of its maximum value on the target surface.

これを図面によって説明すると、第9図はターゲット支
持台5に内蔵される磁石回路の一例であって、バックヨ
ーク8の上に中央円筒磁石9とこれを取り囲んで環状磁
石10が配置されている。この磁石回路の位置と8えと
の関係を示したグラフが第10図である。ここで表われ
る強磁界a域を平面図で示すと第11図のとおりで、そ
の領域はターゲット表面積の35%である。
To explain this with the help of drawings, FIG. 9 shows an example of a magnet circuit built into the target support base 5, in which a central cylindrical magnet 9 and an annular magnet 10 are arranged on the back yoke 8, surrounding the central cylindrical magnet 9. . FIG. 10 is a graph showing the relationship between the position of this magnet circuit and the number 8. The strong magnetic field a region appearing here is shown in a plan view as shown in FIG. 11, and this region is 35% of the target surface area.

この環状の強磁界領域に前述のガスプラズマが集まり、
環状エロージョン領域となる。
The aforementioned gas plasma gathers in this annular strong magnetic field region,
This becomes an annular erosion area.

第12図は各磁石が角型の場合の例で、第13図はその
8乳の分布グラフ、第14図は同強磁性領域の平面図で
、その領域はターゲット表面積の32%である。   
  ゛ ターゲットの寿命はこの環状エロージョン領域の深さが
ターゲット支持台またはターゲットバックプレートに達
するまでであり、使用不能となったター、ゲットはエロ
ージョン領域以外の未使用部分が多く残留する。
FIG. 12 shows an example in which each magnet is rectangular, FIG. 13 is a distribution graph of eight magnets, and FIG. 14 is a plan view of the same ferromagnetic region, which is 32% of the target surface area.
``The life of a target is until the depth of this annular erosion area reaches the target support stand or target back plate, and a target that is no longer usable will have many unused parts remaining outside the erosion area.

また、スパッタされる領域が強磁界領域であるエロージ
ョン領域に限定されるため、薄膜生成速度を低下させる
原因にもなっている。
Furthermore, since the region to be sputtered is limited to the erosion region, which is a strong magnetic field region, this also causes a reduction in the thin film production rate.

そこで、本発明ではターゲットの未使用領域が少なく、
成膜速度の大きいマグネトロンスパッタ装置を提供せん
とするものである。
Therefore, in the present invention, the unused area of the target is small and
It is an object of the present invention to provide a magnetron sputtering device with a high film formation rate.

[問題点を解決するための手段] 本発明は、真空容器内に配置されたターゲットと、ター
ゲット表面近傍に磁界を発生する手段を備えるマグネト
ロンスパッタ装置において、磁界発生用の磁気回路が、
中央磁石、環状磁石及び中央から外周方向もしくは外周
から中央方向で、かつターゲット表面と平行な1161
1方向を持つ環状磁石より構成されていることを特徴と
するマグネトロンスパッタ装置である。
[Means for Solving the Problems] The present invention provides a magnetron sputtering apparatus comprising a target disposed in a vacuum container and a means for generating a magnetic field near the surface of the target, in which a magnetic circuit for generating the magnetic field comprises:
Central magnet, annular magnet, and 1161 from the center to the outer circumference or from the outer circumference to the center and parallel to the target surface.
This is a magnetron sputtering device characterized by being composed of an annular magnet having one direction.

上記において、中央磁石および各環状磁石が角型に形成
されていてもよい。
In the above, the central magnet and each annular magnet may be formed into a square shape.

かかる磁気回路は、従来の磁気回路に比して、中央から
外周方向もしくは外周から中央方向でかつターゲット表
面と平行な着磁方向を持つ環状磁石をさらに配置するこ
とによって、前記強磁界領域がターゲット表面積の40
%以上ある磁気回路としたものである。
Compared to conventional magnetic circuits, such a magnetic circuit further disposes an annular magnet having a magnetization direction from the center to the outer periphery or from the outer periphery to the center and parallel to the target surface, so that the strong magnetic field region is aligned with the target. 40 of surface area
% or more of the magnetic circuit.

[作用] 本発明は、ターゲット支持台に内蔵される磁気回路によ
って、広い強磁界領域を発生させて、ターゲットの未使
用領域を少なくし、成膜速度を大とする。
[Function] The present invention generates a wide strong magnetic field region using a magnetic circuit built into the target support, thereby reducing the unused region of the target and increasing the film formation rate.

[実施例] 以下、本発明の実施例を図面を参照して詳細に説明す。[Example] Embodiments of the present invention will be described in detail below with reference to the drawings.

本発明はターゲット支持台内の磁気回路の構成に主たる
特徴があり、他は第8図と同様の構造であるから、説明
は磁気回路のみで行なう。
The main feature of the present invention lies in the configuration of the magnetic circuit within the target support, and the rest of the structure is the same as that shown in FIG. 8, so the explanation will be given only with respect to the magnetic circuit.

なお、実施例は代表例を示すもので、本発明の範囲を限
定するものではなく、勿論他にも本発明の範囲内の実施
例は存在する。
Note that the examples are representative examples and do not limit the scope of the present invention, and of course there are other examples within the scope of the present invention.

実施例1 第1図の丸型ターゲット用磁気回路の構成図であり、図
中矢印は磁石の磁化方向を示す。
Example 1 This is a configuration diagram of the magnetic circuit for a round target in FIG. 1, and the arrow in the figure indicates the magnetization direction of the magnet.

磁気回路中心位置にターゲット表面と垂直な@磁方向を
持つ中央磁石11が配置され、その外周位dに、中央磁
石11と@磁方向を逆にした円環状磁石12を配置し、
さらに中央磁石11と円環状磁石12との上部にさし渡
すように、ターゲットの表面に平行かつ外周から中央方
向に着磁方向を持つ環状磁石13を配置する。8はバッ
クヨークで、漏洩磁界を防ぐために磁気回路下面に配置
される。磁気回路に使用する磁石は保磁力が充分に大き
いことが必要である。
A central magnet 11 having a magnetic direction perpendicular to the target surface is arranged at the center of the magnetic circuit, and an annular magnet 12 whose magnetic direction is opposite to that of the central magnet 11 is arranged at the outer circumference d.
Further, an annular magnet 13 is arranged so as to span over the center magnet 11 and the annular magnet 12, parallel to the surface of the target and having a magnetization direction from the outer periphery toward the center. Reference numeral 8 denotes a back yoke, which is placed on the lower surface of the magnetic circuit to prevent leakage magnetic fields. The magnet used in the magnetic circuit needs to have a sufficiently large coercive force.

ターゲット表面は磁気回路上面より12av上方に位置
しており、その面上におけるB1の分布及び強磁界領域
を第2図に示し、第3図は強磁界領域の平面図を示す。
The target surface is located 12 av above the upper surface of the magnetic circuit, and FIG. 2 shows the distribution of B1 and the strong magnetic field region on that surface, and FIG. 3 shows a plan view of the strong magnetic field region.

本実施例での強磁界領域は全ターゲット表面積の47%
である。又、第4図は第1図の場合と@磁方向の異なる
、すなわち環状磁石13の着磁方向が中央から外周方向
にしたものである。
In this example, the strong magnetic field area accounts for 47% of the total target surface area.
It is. Further, in FIG. 4, the magnetic direction is different from that in FIG. 1, that is, the direction of magnetization of the annular magnet 13 is from the center to the outer circumferential direction.

実施例2 第5図は角型ターゲット用磁気回路の構成図であり、磁
気回路中心位置にターゲット表面と垂直な磁化を持つ角
型中央磁石14が配置され、その外周位置に角型中央磁
石14と着磁方向を逆にした角環状磁石15を配置し、
さらに角型中央磁石14と角環状磁石15との上部にさ
し渡すように、ターゲットの表面に平行かつ外周から中
央方向に着磁方向を持つ角環状磁石16を配置する。
Embodiment 2 FIG. 5 is a configuration diagram of a magnetic circuit for a square target, in which a square central magnet 14 having magnetization perpendicular to the target surface is arranged at the center position of the magnetic circuit, and square central magnets 14 are arranged at the outer circumferential position of the square central magnet 14. A square annular magnet 15 with the magnetization direction reversed is arranged,
Further, a square annular magnet 16 is arranged so as to span over the square central magnet 14 and the square annular magnet 15, parallel to the surface of the target and having a magnetization direction from the outer periphery toward the center.

8はバックヨークである。8 is a back yoke.

第6図は第5図のA−A″線上B、Lの分布及び強磁界
領域を示すグラフで、第7図はその強磁界領域の平面図
である。本実施例での強磁界領域は全ターゲット表面積
の42%である。
Fig. 6 is a graph showing the distribution of B and L on line A-A'' in Fig. 5 and the strong magnetic field region, and Fig. 7 is a plan view of the strong magnetic field region. This is 42% of the total target surface area.

[発明の効果] 本発明のマグネトロンスパッタ装置は、ターゲット表面
の強磁界領域が従来品と比較して約1.3〜1.8倍と
なり、スパッタされるエロージョン領域がこれに従って
大きくなって、ターゲットの未使用部分が減少し、利用
効率が向上し、さらに高い成膜速度が得られる。したが
って、半導体集積回路、磁気記録媒体の製造に適用して
すぐれた効果を得ることができる。又、本発明における
磁気回路は強磁場を広い閣囲で発生するので、磁気回路
の構成そのものは、例えば磁気浮上MRIの磁気回路等
にも適用できる。
[Effects of the Invention] In the magnetron sputtering apparatus of the present invention, the strong magnetic field area on the target surface is approximately 1.3 to 1.8 times larger than that of conventional products, and the erosion area to be sputtered is correspondingly large. The unused portion of the film is reduced, the utilization efficiency is improved, and a higher deposition rate can be obtained. Therefore, excellent effects can be obtained when applied to the manufacture of semiconductor integrated circuits and magnetic recording media. Further, since the magnetic circuit according to the present invention generates a strong magnetic field over a wide area, the structure of the magnetic circuit itself can be applied to, for example, a magnetic circuit for magnetic levitation MRI.

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

第1図は本発明の実施例の磁気回路の構成図、第2図は
同Bトの分布グラフ、第3図は同強磁界領域の平面図、
第4図は第1図の変形例の構成図、第5図は他の実施例
の磁気回路の構成図、第6図は同8Nの分布グラフ、第
7図は同強磁界領域の平面図、第8図はマグネトロンス
パッタ装置の概念図、第9図は従来の磁気回路の構成図
、第10図は同B1の分布グラフ、第11図は同強磁界
領域の平面図、第12図は他の従来例の磁気回路の構成
図、第13図は同B、の分布グラフ、第14図は同強磁
界領域の平面図である。
FIG. 1 is a configuration diagram of a magnetic circuit according to an embodiment of the present invention, FIG. 2 is a distribution graph of B, and FIG. 3 is a plan view of the strong magnetic field region.
Fig. 4 is a block diagram of a modification of Fig. 1, Fig. 5 is a block diagram of a magnetic circuit of another embodiment, Fig. 6 is a distribution graph of 8N, and Fig. 7 is a plan view of the strong magnetic field region. , Fig. 8 is a conceptual diagram of a magnetron sputtering device, Fig. 9 is a configuration diagram of a conventional magnetic circuit, Fig. 10 is a distribution graph of B1, Fig. 11 is a plan view of the strong magnetic field region, and Fig. 12 is a diagram of a conventional magnetic circuit. FIG. 13 is a diagram showing the configuration of another conventional magnetic circuit, and FIG. 13 is a distribution graph of B, and FIG. 14 is a plan view of the strong magnetic field region.

Claims (1)

【特許請求の範囲】 (1)真空容器内に配置されたターゲットと、ターゲッ
ト表面近傍に磁界を発生する手段を備えるマグネトロン
スパッタ装置において、磁界発生用の磁気回路が、中央
磁石、環状磁石及び中央から外周方向もしくは外周から
中央方向で、かつターゲット表面と平行な着磁方向を持
つ環状磁石より構成されていることを特徴とするマグネ
トロンスパッタ装置。(2)各磁石が角型に構成されて
いる特許請求の範囲第(1)項記載のマグネトロンスパ
ッタ装置。 (3)強磁界領域が、ターゲット表面積の40%以上あ
る磁気回路をもつ特許請求の範囲第(1)項又は第(2
)項記載のマグネトロンスパッタ装置。
[Scope of Claims] (1) In a magnetron sputtering apparatus comprising a target disposed in a vacuum container and means for generating a magnetic field near the surface of the target, a magnetic circuit for generating a magnetic field includes a central magnet, an annular magnet and a central magnet. 1. A magnetron sputtering apparatus comprising an annular magnet having a magnetization direction parallel to a target surface, either from the outer periphery or from the outer periphery to the center. (2) The magnetron sputtering apparatus according to claim (1), wherein each magnet has a rectangular shape. (3) Claim (1) or (2) in which the strong magnetic field region has a magnetic circuit that is 40% or more of the target surface area.
) The magnetron sputtering device described in item 2.
JP62263655A 1987-10-21 1987-10-21 Magnetron sputtering equipment Expired - Fee Related JPH0826454B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62263655A JPH0826454B2 (en) 1987-10-21 1987-10-21 Magnetron sputtering equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62263655A JPH0826454B2 (en) 1987-10-21 1987-10-21 Magnetron sputtering equipment

Publications (2)

Publication Number Publication Date
JPH01108375A true JPH01108375A (en) 1989-04-25
JPH0826454B2 JPH0826454B2 (en) 1996-03-13

Family

ID=17392488

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62263655A Expired - Fee Related JPH0826454B2 (en) 1987-10-21 1987-10-21 Magnetron sputtering equipment

Country Status (1)

Country Link
JP (1) JPH0826454B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1697556A2 (en) * 2003-11-05 2006-09-06 Dexter Magnetic Technologies, Inc. Rotating sputtering magnetron

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5881969A (en) * 1981-11-06 1983-05-17 Kokusai Electric Co Ltd Sputter source of magnetron sputtering
JPS58199862A (en) * 1982-05-18 1983-11-21 Tdk Corp Magnetron type sputtering device
JPS60116774A (en) * 1983-11-30 1985-06-24 Nippon Texas Instr Kk Sputtering device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5881969A (en) * 1981-11-06 1983-05-17 Kokusai Electric Co Ltd Sputter source of magnetron sputtering
JPS58199862A (en) * 1982-05-18 1983-11-21 Tdk Corp Magnetron type sputtering device
JPS60116774A (en) * 1983-11-30 1985-06-24 Nippon Texas Instr Kk Sputtering device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1697556A2 (en) * 2003-11-05 2006-09-06 Dexter Magnetic Technologies, Inc. Rotating sputtering magnetron
EP1697556A4 (en) * 2003-11-05 2008-09-17 Dexter Magnetic Technologies I Rotating sputtering magnetron

Also Published As

Publication number Publication date
JPH0826454B2 (en) 1996-03-13

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