JPS596377A - Magnetron sputtering apparatus - Google Patents

Magnetron sputtering apparatus

Info

Publication number
JPS596377A
JPS596377A JP11553982A JP11553982A JPS596377A JP S596377 A JPS596377 A JP S596377A JP 11553982 A JP11553982 A JP 11553982A JP 11553982 A JP11553982 A JP 11553982A JP S596377 A JPS596377 A JP S596377A
Authority
JP
Japan
Prior art keywords
anode
target
magnets
pair
cathode 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.)
Pending
Application number
JP11553982A
Other languages
Japanese (ja)
Inventor
Yuji Haji
土師 裕二
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.)
Tokin Corp
Original Assignee
Tohoku Metal Industries 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 Tohoku Metal Industries Ltd filed Critical Tohoku Metal Industries Ltd
Priority to JP11553982A priority Critical patent/JPS596377A/en
Publication of JPS596377A publication Critical patent/JPS596377A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/32Gas-filled discharge tubes
    • H01J37/34Gas-filled discharge tubes operating with cathodic sputtering
    • H01J37/3402Gas-filled discharge tubes operating with cathodic sputtering using supplementary magnetic fields
    • H01J37/3405Magnetron sputtering
    • H01J37/3408Planar magnetron sputtering

Abstract

PURPOSE:To provide a magnetron sputtering apparatus enlarged in the available utilizing region of a target, by making the mutual positional relation of a pair of magnets arranged in the vicinity of the surface of a cathode target opposed to an anode variable. CONSTITUTION:A pair or more of magnets 6a, 6b of which mutually different magnetic pole surfaces are directed to an anode are arranged in the vicinity of the surface of a cathode target 2 opposed to the anode arranged in a vacuum container. These magnets 6a, 6b for generating magnetic fields are formed into a mutually movable structure or at leastone of each pair of the magnets 6a, 6b is made exchangeable with a magnet different in a size. By this method, sputtered regions 9, 9' are enlarged and the usable time of the same target 2 can be prolonged. In addition, the structural irregularity of a product can be suppressed.

Description

【発明の詳細な説明】 本発明は、電界と磁界とが直交した場におけるマグネト
ロン放電を利用したマグネトロンスミ9ツタ装置に関す
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetron sumi9 ivy device that utilizes magnetron discharge in a field where an electric field and a magnetic field are perpendicular to each other.

マグネトロンスパッタ装置においては、互に対向する陰
極ターゲット及び陽極間の電界に対して直交する磁界が
、陰極ターゲットの陽極仝の対向面の近傍に得られるよ
うに、陰極ターゲットの裏面側等に、一対の磁石が配置
されるのが、普通である。そして、陽極の陰極ターゲッ
トへの対向面に被膜を形成すべき目的物体が配置される
In a magnetron sputtering device, a pair is installed on the back side of the cathode target, etc. so that a magnetic field perpendicular to the electric field between the cathode target and the anode, which face each other, is obtained near the opposing surfaces of the cathode target and the anode. It is common for a number of magnets to be placed. Then, a target object on which a film is to be formed is placed on the surface of the anode facing the cathode target.

このようなマグネトロンスパッタ装置においては、陰極
に用いられるターゲットのスパッタ消費面の形状は、上
記一対の磁石の設置状態に対応しておシ、この一対の磁
石の発生する磁界にょシ囲まれた領域がホロウ(hol
low)状に消費された形状となる。
In such magnetron sputtering equipment, the shape of the sputter consuming surface of the target used as the cathode corresponds to the installation state of the pair of magnets, and the shape is the area surrounded by the magnetic field generated by the pair of magnets. is hollow
It becomes a shape that is consumed in a low) manner.

当該ターケ8ットは厚さ方向の一部が消費されるまで使
用されるが、その一部が消費しつくされれば、たとえそ
の他の大部分が残存していても、全体を交換しなければ
ならず、その有効使用量はターゲット重量全体の15〜
25チにみため場合が多かった。
The target can be used until a part of the thickness is consumed, but once that part is consumed, the entire piece must be replaced even if most of the other parts remain. Of course, its effective usage amount is 15 to 15% of the total target weight.
There were many cases where it was seen at around 25 cm.

当該ターケ9ットのロット間の「ばらつき」にょる製品
の歩留シを向上させる為、さらには経済性を向上させる
為に、ターゲットの有効利用面積を広げる方法が望まれ
ている。
In order to improve the yield of products due to "variations" between lots of targets, and furthermore to improve economic efficiency, a method of expanding the effective usable area of targets is desired.

本発明の目的は、ターゲットの有効利用面積を広げるこ
とができるマグネトロンスパッタ装置を提供し、ターケ
9ットの経済性を向上せしめることにある。
An object of the present invention is to provide a magnetron sputtering apparatus that can expand the effective use area of a target, and to improve the economic efficiency of a target.

本発明によれば、排気系に接続されている真空容器内に
対向するように配置された陰極ターゲット及び陽極と、
該陰極ターケ9ット及び陽極間に接続される電源と、上
記陰極ターダウトの上記陽極への対向面の近傍に上記電
源による上記陰極ターゲット及び陽極間の電界に対して
直交する磁界が得られるように、互に異なる磁極面を上
記陽極に向けて少なくとも一対配置された磁石とを備え
According to the present invention, a cathode target and an anode are arranged to face each other in a vacuum container connected to an exhaust system;
A power supply connected between the cathode target 9 and the anode, and a magnetic field perpendicular to the electric field between the cathode target and the anode caused by the power supply near the surface of the cathode doubt facing the anode. and at least one pair of magnets arranged with mutually different magnetic pole faces facing the anode.

上記陽極の上記陰極ターゲットへの対向面に目的物体を
配置するようにしたマグネトロンスパッタ装置において
、上記一対の磁石の相対位置関係を可変としたことを特
徴とするマグネトロンスパッタ装置が得られる。
A magnetron sputtering apparatus is obtained in which a target object is placed on the surface of the anode facing the cathode target, characterized in that the relative positional relationship between the pair of magnets is variable.

以下1図面を参照して説明する。This will be explained below with reference to one drawing.

、第1図を参照すると、従来のマグネトロンスパッタ装
置は、真空容器1内に対向するように配置された陰極タ
ーゲット2及び陽極3と、陰極ターゲット2及び陽極3
間に接続される直流の高電圧源5(この代シに高周波の
高電圧源を用いてもよい。)と、陰極ターゲット2の陽
極3に対向する第1の表面の近傍に高電圧源5による陰
極ターケ゛ット2及び陽極3間の電界に対して直交する
磁界が得られるように、互に異なる磁極面を陽極3に向
けて一対配置された環状磁石6a、6bとを備え、陽極
3の陰極ターケ8ット2への対向面に目的物体4を配置
するようにしたものである。
Referring to FIG. 1, the conventional magnetron sputtering apparatus includes a cathode target 2 and an anode 3 arranged to face each other in a vacuum chamber 1, and a cathode target 2 and an anode 3 arranged to face each other in a vacuum chamber 1.
A DC high voltage source 5 (a high frequency high voltage source may be used instead) connected between In order to obtain a magnetic field orthogonal to the electric field between the cathode target 2 and anode 3, a pair of annular magnets 6a and 6b are arranged with different magnetic pole faces facing the anode 3, The target object 4 is placed on the surface facing the target 8t 2.

真空容器1には、ロータリーポンプ、拡散ポンプ等の排
気系8が接続され、さらにはMガス導入路系統(図示せ
ず)も接続されている。また、上述した一対の環状磁石
6a 、6bは、陰極ターゲット2の陽極3に対向する
第1の表面とは反対側の第2の表面(裏面)側に配置さ
れている。また。
An exhaust system 8 such as a rotary pump or a diffusion pump is connected to the vacuum container 1, and an M gas introduction path system (not shown) is also connected thereto. Further, the pair of annular magnets 6a and 6b described above are arranged on the second surface (back surface) side of the cathode target 2, which is opposite to the first surface facing the anode 3. Also.

一対の環状磁石6a、6bは底部磁性材6cに固定され
ている。このような一対の磁石6a、6bから発生する
磁束Φは、陰極ターゲット2の陽極3への対向面(第1
の表面)の近傍で電界と直交するようにし、しかも電子
に磁界内で旋回運動をさせるために放射状を形成するよ
うに構成しである。
A pair of annular magnets 6a and 6b are fixed to the bottom magnetic material 6c. The magnetic flux Φ generated from such a pair of magnets 6a and 6b is generated on the surface of the cathode target 2 facing the anode 3 (the first
It is configured to be perpendicular to the electric field near the surface of the magnetic field, and to form a radial shape in order to cause the electrons to rotate within the magnetic field.

とのマグネトロンスパッタ装置において、適当な負電位
を陰極ターゲット2に供給し、磁界を印加すると、陰極
ターゲット2と陽極3との間の空間に、いわゆるマグネ
トロン放電が生じる。すなわち、とのマグネトロンスパ
ッタ装置は、陰極ターゲット2の上記第1の表面(陽極
3への対向面)の近傍にプラズマを集束させて高密度の
プラズマとするために電界に対して直交する磁界を用い
In the magnetron sputtering apparatus, when a suitable negative potential is supplied to the cathode target 2 and a magnetic field is applied, a so-called magnetron discharge occurs in the space between the cathode target 2 and the anode 3. In other words, the magnetron sputtering apparatus of 2008 applies a magnetic field orthogonal to the electric field in order to focus the plasma near the first surface (the surface facing the anode 3) of the cathode target 2 to form a high-density plasma. use.

しかもこの直交電磁界によシ放出電子に陰極ターゲット
2の上記第1の表面近傍を連続的に旋回運動させるよう
にしたものである。一方、プラズマ中の正イオンの陰極
ターrヮト2への衝突によシ陰極材から飛散されるスパ
ッタ粒子7は目的物体4の表面に付着し、被膜が形成さ
れる。また、このスパッタ装置では電子の運動軌跡が磁
石6a。
Furthermore, the orthogonal electromagnetic field causes the emitted electrons to continuously rotate in the vicinity of the first surface of the cathode target 2. On the other hand, sputtered particles 7 scattered from the cathode material due to the collision of positive ions in the plasma with the cathode tar 2 adhere to the surface of the target object 4, forming a film. Furthermore, in this sputtering apparatus, the locus of movement of electrons is the same as the magnet 6a.

6bによシ長くなシ、空間に電子を長くとどめて放電を
生じ易くしているが、電子が陽極3にぶつかる割合が少
なく陽極3の温度はほとんど上昇しない。
6b is longer so that electrons remain in the space for a longer time to facilitate discharge, but the ratio of electrons hitting the anode 3 is small and the temperature of the anode 3 hardly rises.

第2図を参照すると、第1図における陰極ターj” ツ
) 2が示されている。放射状の磁束Φによってターゲ
ット2のスパッタ領域9(内外の破線で囲まれた部分)
が決まシ、その環状のスパッタ領域9の中心線が最深ス
パッタ線10となる。一方。
Referring to FIG. 2, the cathode target 2 in FIG.
Once this is determined, the center line of the annular sputter region 9 becomes the deepest sputter line 10. on the other hand.

電子は上述の環状スフ9ツタ領域9上の空間を符号11
で示したように旋回運動をする。ス・ヤツタリングター
ダット2は第2図に示すように磁界によシ囲まれた領域
に凝集された陽イオンによシ表面をたたかれその個所を
飛ばすが、従来のスパッタ装置ではターrウド2の有効
利用範囲を拡げる手段がとられていない。
The electrons occupy the space above the above-mentioned annular suffix 9 ivy region 9 with the symbol 11
Performs a turning motion as shown in . As shown in Fig. 2, the sputtering target 2 hits the surface of the sputtering surface with positive ions that are aggregated in a region surrounded by a magnetic field and scatters the cations. No measures have been taken to expand the scope of Udo 2's effective use.

本発明は、マグネトロンスパッタリングを行った際の厚
さ方向の消費に分布の生じる事に注目し。
The present invention focuses on the fact that there is a distribution in consumption in the thickness direction when magnetron sputtering is performed.

最も消費される部分10を移動させる事によシ。By moving the most consumed part 10.

ターゲット2の有効利用範囲を拡げようとするものであ
る。このため、スi!−)夕装置の磁界発生用の一対の
磁石6a 、6bを相対的に移動可能な構造としたシ、
一対の磁石6a、6bのうち少なくとも一方を大きさの
異なる磁石に真空容器1内において交換可能な構造とす
るものである。
This is an attempt to expand the range of effective use of Target 2. For this reason, Sui! -) A system in which a pair of magnets 6a and 6b for generating a magnetic field of the evening device are configured to be relatively movable;
The structure is such that at least one of the pair of magnets 6a and 6b can be replaced with a magnet of a different size within the vacuum vessel 1.

以下に本発明の実施例を図面を用いて説明する。Embodiments of the present invention will be described below with reference to the drawings.

第3図にスパッタリング前の当該ターケ゛ット2の断面
図を示し、第4図にス・fツタリングの進行中の同部位
の断面形状を示す。第4図において、スパッタリングは
マグネット間中央部で最も進行している。
FIG. 3 shows a cross-sectional view of the target 2 before sputtering, and FIG. 4 shows a cross-sectional shape of the same portion while sputtering is in progress. In FIG. 4, sputtering is most advanced in the center between the magnets.

第5図はAtをターゲットとしたス・ぐツタリングの進
行深さくmax)と印加エネルギー(MJ:メがジュー
ル)の関係を示す。第6図は二重環状の外側磁石6bを
中央寄シに移動したシ、外側磁石6bを径の小さなもの
に交換して、ターゲット2の最深スパッタ線10を中央
寄りに移した後のターゲット20部分の断面図であシ、
第7図にその移動距離とターダウトの消費重量の変化率
を示した。
FIG. 5 shows the relationship between the progress depth (max) of the suction ring targeting At and the applied energy (MJ: medium joule). Figure 6 shows the target 20 after the double annular outer magnet 6b has been moved closer to the center, the outer magnet 6b has been replaced with a smaller diameter one, and the deepest sputtered line 10 of the target 2 has been moved closer to the center. A cross-sectional view of the part.
Figure 7 shows the distance traveled and the rate of change in the weight consumed by the tardoubt.

すなわち2本発明において、 AAメタ−ットを用いア
ルゴン雰囲気でスパッタリングしたが、一対の磁石6a
、6b間の中央部のス・母ツタリングが最も進行し、第
5図に示すように印加エネルギーに比例してゆく。次に
、第6図に示す如く磁力線をΦの状態からΦ′の状態に
変化させて再度ス・ぐツタリングした所、十印で示すよ
うに新らしくス・やツタリングされた範囲9′が広がシ
、第7図に示すように期待された効果が確認された。
That is, in the second invention, sputtering was carried out in an argon atmosphere using AA metal, but a pair of magnets 6a
, 6b progresses the most, and as shown in FIG. 5, it progresses in proportion to the applied energy. Next, as shown in Figure 6, when the lines of magnetic force were changed from the state of Φ to the state of Φ' and strutting was performed again, the new strutted area 9' became wider as shown by the cross mark. However, as shown in Figure 7, the expected effects were confirmed.

以上説明したように1本発明によれば、マグネトロンス
・やツタ装置の一対の磁石の相対位置関係を可変とした
ことによシ、使用ターダットの有効利用領域を拡げる事
が可能になり、経済的となる。
As explained above, according to the present invention, by making the relative positional relationship between the pair of magnets in the magnetron and the vine device variable, it is possible to expand the range of effective use of the used TARDIT, thereby making it possible to achieve economical become a target.

特に、真空容器内において、一対の磁石を移動可能な構
造又は一対の磁石のうち少なくとも一方を大きさの異な
る磁石に交換可能な構造とすることによシ同一ターダッ
トの使用可能時間を延ばす事も可能になり、製品の構造
上のバラツキを抑える手段を提供する事が出来、非常に
有用である。
In particular, by creating a structure in which a pair of magnets can be moved within a vacuum container, or a structure in which at least one of the pair of magnets can be replaced with a magnet of a different size, the usable life of the same TARDAT can be extended. This makes it possible to provide a means to suppress structural variations in products, which is extremely useful.

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

第1図は従来のマグネトロンスパッタ装置の概略図、第
2図は第1図のマグネトロンスi’?ツタ装置のターゲ
ットの表面状態を示した斜視図、第3図、第4図及び第
6図はそれぞれ本発明の実施例におけるターケ゛ット部
分の断面図、第5図は印加エネルギーとスパッタリング
進行厚さくmay) (D FJI係を示した図、第7
図は磁石間の間隔の変化率とターゲット重量変化率の関
係を表わした図である。 1・・・真空容器、2・・・陰極ターrウド、3・・・
陽極。 4・・・目的物体、5・・・電源+6a及び6b・・・
一対の磁石、7・・・ス・ぐツク粒子、8・・・排気系
、9・・・環状スパッタ領域、10・・・最深スパッタ
線、11・・・電子の軌跡。 第2図 第5図 [D加エネルヤー(MJ)
FIG. 1 is a schematic diagram of a conventional magnetron sputtering apparatus, and FIG. 2 is a diagram of the magnetron sputter i'? FIGS. 3, 4, and 6 are perspective views showing the surface condition of the target of the ivy device. FIGS. 3, 4, and 6 are sectional views of the target portion in an embodiment of the present invention, and FIG. ) (D Diagram showing FJI staff, No. 7
The figure shows the relationship between the rate of change in the spacing between magnets and the rate of change in target weight. 1... Vacuum vessel, 2... Cathode turret, 3...
anode. 4...Target object, 5...Power supply +6a and 6b...
A pair of magnets, 7... S.G. particles, 8. Exhaust system, 9. Annular sputtering region, 10. Deepest sputtered line, 11. Trajectory of electrons. Figure 2 Figure 5 [D addition energy (MJ)

Claims (1)

【特許請求の範囲】 1、排気系に接続されている真空容器内に対向するよう
に配置された陰極ターゲット及び陽極と。 該陰極ターケ゛ット及び陽極間に接続される電源と。 上記陰極ターゲットの上記陽極への対向面の近傍に上記
電源による上記陰極ターゲット及び陽極間の電界に対し
て直交する磁界が得られるように。 互に異なる磁極面を上記陽極に向けて少なくとも一対配
置された磁石とを備え、上記陽極の上記陰極ターゲット
への対向面に目的物体を配置するようにしたマグネトロ
ンスパッタ装置において、上記一対の磁石の相対位置関
係を可変としたことを特徴とするマグネトロンスパッタ
装置。
[Claims] 1. A cathode target and an anode arranged to face each other in a vacuum container connected to an exhaust system. and a power source connected between the cathode target and the anode. A magnetic field perpendicular to the electric field between the cathode target and the anode caused by the power source is obtained near the surface of the cathode target facing the anode. A magnetron sputtering apparatus comprising at least one pair of magnets disposed with mutually different magnetic pole faces facing the anode, and a target object is disposed on a surface of the anode facing the cathode target, wherein the magnetron sputtering apparatus comprises: A magnetron sputtering device characterized by variable relative positional relationship.
JP11553982A 1982-07-05 1982-07-05 Magnetron sputtering apparatus Pending JPS596377A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11553982A JPS596377A (en) 1982-07-05 1982-07-05 Magnetron sputtering apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11553982A JPS596377A (en) 1982-07-05 1982-07-05 Magnetron sputtering apparatus

Publications (1)

Publication Number Publication Date
JPS596377A true JPS596377A (en) 1984-01-13

Family

ID=14665031

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11553982A Pending JPS596377A (en) 1982-07-05 1982-07-05 Magnetron sputtering apparatus

Country Status (1)

Country Link
JP (1) JPS596377A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4606806A (en) * 1984-05-17 1986-08-19 Varian Associates, Inc. Magnetron sputter device having planar and curved targets
EP1215302A1 (en) * 1999-07-06 2002-06-19 Applied Materials, Inc. Sputtering device and film forming method

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4606806A (en) * 1984-05-17 1986-08-19 Varian Associates, Inc. Magnetron sputter device having planar and curved targets
EP1215302A1 (en) * 1999-07-06 2002-06-19 Applied Materials, Inc. Sputtering device and film forming method
EP1215302A4 (en) * 1999-07-06 2007-11-07 Applied Materials Inc Sputtering device and film forming method

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