JPS58189370A - Sputtering device - Google Patents

Sputtering device

Info

Publication number
JPS58189370A
JPS58189370A JP7024582A JP7024582A JPS58189370A JP S58189370 A JPS58189370 A JP S58189370A JP 7024582 A JP7024582 A JP 7024582A JP 7024582 A JP7024582 A JP 7024582A JP S58189370 A JPS58189370 A JP S58189370A
Authority
JP
Japan
Prior art keywords
target
sputtering
magnetic field
magnetic
generating means
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
JP7024582A
Other languages
Japanese (ja)
Other versions
JPS6343465B2 (en
Inventor
Sadao Kadokura
貞夫 門倉
Kazuhiko Honjo
和彦 本庄
Masahiko Naoe
直江 正彦
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.)
Teijin Ltd
Original Assignee
Teijin 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 Teijin Ltd filed Critical Teijin Ltd
Priority to JP7024582A priority Critical patent/JPS58189370A/en
Publication of JPS58189370A publication Critical patent/JPS58189370A/en
Publication of JPS6343465B2 publication Critical patent/JPS6343465B2/ja
Granted 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

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Electrodes Of Semiconductors (AREA)
  • Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)
  • Physical Vapour Deposition (AREA)

Abstract

PURPOSE:To improve the performance of a sputtering device by providing magnetic field generating means on the rear surface side of a target, and using a soft magnetic material having high magnetic permeability in constituting an end part of a magnetic pole of said means facing the target. CONSTITUTION:Cylindrical frame bodies 31, 32 which consist of a soft magnetic material of high magnetic permeability having the convergent forward end faces facing each other are disposed on the rear surfaces at the ends on the target T1, T2 sides in target holders 11, 12, and permanent magnets 33, 34 are disposed in tight contact with the root end faces of the bodies 31, 32. The magnetic poles thereof are so arranged that the different poles face each other. The inside of a vacuum vessel 10 is evacuated thoroughly through an evacuation port 40 with an evacuation system, whereafter a sputtering gas is introduced from a gas introduction system through an introduction port 50. Sputtering electric power is supplied to shielding rings 13, 14 and the targets T1, T2 from a sputtering power source 60, whereby sputtering is accomplished and the thin films conforming to the targets T1, T2 are formed on a substrate 20. the uniform thin films are thus formed uniformly and widely at a low temp. in high speed.

Description

【発明の詳細な説明】 本発明は、スパッタ装置の改良、更に計しくに、灼向タ
ーケット式スパッタ装置の如くターゲットの背1III
体にフラズマ形成のための磁界発生手段を設けたスパッ
タ装置の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention aims to improve sputtering equipment, and furthermore, to improve sputtering equipment such as a target sputtering equipment such as a target sputtering equipment.
The present invention relates to an improvement of a sputtering apparatus in which a magnetic field generating means for forming a plasma is provided in the body.

近年、姻究、開免の盛んな超LSI 、光麹伯用憬籠デ
バイス、尚M、′&度記録用素子などでは、^空蒸、+
l1lI法ではとCも作製できないような畠融点あるい
はY6性的な材料の腺をその粕成9寸法。
In recent years, research and development of ultra-LSIs, optical cage devices, and devices for recording degrees are based on air vaporization, +
It is possible to create glands of materials with a melting point or Y6 temperature that cannot be produced using the I1I method.

ネ1性を制御しながら作製するという強い要望がk・9
、どのような羽科でもほとんどの基板上に膜形成ができ
る技術としてスパッタ法が足置され、その欠点の克服の
ために精力的な研究、開発がなさねている。そして、そ
の方向it市達化。
There is a strong desire to manufacture k・9 while controlling the
Sputtering has been widely accepted as a technology that can form films on most substrates for any species of feathers, and vigorous research and development efforts are currently underway to overcome its drawbacks. And in that direction, it will become a city.

低温化にあり、櫨々の方式のスパッタ法について勢既に
多くの払案がある。
With the trend toward lower temperatures, there are already many proposals for the Hashira-style sputtering method.

本発明者の一人も、先に萬速、低温のスパッタができる
上、磁性材料にも適用できるスパッタ方式として対向タ
ーゲット式スパッタ装置を徒事し九(「応用物理」第4
8巻第6号(197a)P558〜P559 )。この
対向ターゲット式スパッタ装置tは′a1図に示すよう
に構成される。すなわち、従来の真空槽内圧基板とター
ゲットを対向場ぜた2@スパツタ装置と異なり、真空槽
10内に一対のターゲットT++Txt−スパッタされ
るスパッタ面T1s、Tomが空間を隔てて平行に対面
するように配置すると共に、基板20はターゲラ)T1
.T、の側方に設けた基板ホルダー21vCよりターゲ
ラF ”I + ”!の空間の側方に該空間に刈囲する
ように配置する。そして、真空槽lOJノ回りに設けた
コイル、(0によりスパッタ凹Tl s 、 72 s
に垂直な方向の磁界Hを発生させるようにしである。な
お、図の11,12i1鉄から16ターグノトホルダー
、13.14は瓶禮のた め ぴン 7− ル ト で
 1(卜 る 。
One of the inventors of the present invention also developed a facing target sputtering system as a sputtering method that can perform multi-speed, low-temperature sputtering and can also be applied to magnetic materials.
Vol. 8, No. 6 (197a) P558-P559). This facing target type sputtering apparatus t is constructed as shown in Figure 'a1. That is, unlike the conventional 2@ sputtering apparatus in which a vacuum chamber internal pressure substrate and a target are placed in opposing fields, a pair of targets T++Txt- sputtering surfaces T1s and Tom to be sputtered are placed in the vacuum chamber 10 so that they face each other in parallel across a space. and the substrate 20 is T1
.. Targetera F "I +" from the board holder 21vC installed on the side of T. It is placed on the side of the space so as to surround the space. Then, the coil provided around the vacuum chamber lOJ, (0 causes a sputter recess Tl s, 72 s
This is to generate a magnetic field H in a direction perpendicular to . In addition, in the figure, 11, 12i1 iron to 16 terminal holder, 13.14 are pins 7-root for bottling.

従って、図示省略した排気系により排気口40を通して
真空槽10内を排気した後、V示省略したガス導入系か
ら導入口s o ′(r通してアルゴン等のスパッタガ
スを導入し、図示の如く自流電源からなるスパッタ電源
60によりシールド13.14従って真空槽10を陽極
(接地)K。
Therefore, after evacuating the inside of the vacuum chamber 10 through the exhaust port 40 by an exhaust system (not shown), a sputtering gas such as argon is introduced from the gas introduction system (not shown) through the inlet s o '(r). The shield 13.14 and therefore the vacuum chamber 10 are connected to the anode (ground) K by a sputtering power source 60 consisting of a self-current power source.

ターゲット’r、 j T2 を陰極にしてスパッタ電
力を供給し、コイル30により前述の磁界Hを発生させ
ることKよりスパッタが行なわれ、基&20上にターゲ
ラ) TI * T*に対応した組成の¥lI膜が形成
される。
Sputtering is performed by supplying sputtering power using the target 'r, j T2 as a cathode and generating the above-mentioned magnetic field H using the coil 30, and sputtering is performed on the base &20 with a composition corresponding to TI*T*. A II film is formed.

この際、前述の構成によりスパッタ面Tl s 、TI
 1に垂直に磁界が印加されているので、対向するター
ゲットTI r ’r2間の空間内に高エネルギー電子
が閉じ込められ、ここでのスパッタガスのイオン化が促
進されてスパッタ速度が高くな9高速の膜形成ができる
。その上、基&20は従来のスパッタ装置の如くターゲ
ットに対向せずターゲラ) T1 r T2の側方に配
置されているので、基板20上への高いエネルギーを有
するイオンや電子の衝突がほとんどなくなり、かつター
ゲラ)T、、T、からの熱輻射も小さく基板温度の上昇
の小さい、よって低温の膜形成ができる。更に磁界は全
体としてターゲラ) T、 、 ’r、の垂直方向に印
加しであるので、ターゲット−0−に磁性材料を用いて
も有効に磁界が作用し、高速膜形成ができる。
At this time, due to the above-mentioned configuration, the sputtering surfaces Tl s , TI
Since a magnetic field is applied perpendicular to 1, high-energy electrons are confined in the space between the opposing targets TIr'r2, and ionization of the sputtering gas is promoted here, resulting in a high sputtering rate. Can form a film. Furthermore, since the base 20 is placed on the side of the target (T1 r T2) instead of facing the target as in conventional sputtering equipment, collisions of high-energy ions and electrons onto the substrate 20 are almost eliminated. In addition, thermal radiation from T, , T, is small, and the rise in substrate temperature is small, so that low-temperature film formation is possible. Furthermore, since the magnetic field is applied in the perpendicular direction to the target layer T, , 'r as a whole, the magnetic field acts effectively even if a magnetic material is used for the target 0-, allowing high-speed film formation.

本発明は、上述の対向ターゲット式スノくツタ装置の改
良を主な目的としたもの、すなわち、〔1〕ターゲツト
のスパッタされる面を広くかつ均一にしてターゲットの
使用効率を向上させると共に、〔2〕ターゲツトの冷却
効率を向上させ、低温かつ高速に膜形成する舵力をさら
に改番し、〔3〕その上対向するターゲットの空間ヲ折
!大して生オ性を高めることを可能とした、〔4〕コン
パクトで安価な構成の対向ターゲット式スノ(ツタ装置
を提供することを主目的としたものであるか、他の四種
のターゲットの背面に磁界発生手段を設けたスパッタ装
置にも効果的に適用できiものである。
The main objectives of the present invention are to improve the above-mentioned opposed target type snow sputtering device, namely, [1] improve the use efficiency of the target by widening and uniformly sputtering the surface of the target; 2) Improve the cooling efficiency of the target, further change the steering force to form a film at low temperature and high speed, and [3] Moreover, fold the space of the opposing target! [4] Compact and inexpensive configuration of facing target type snowball (mainly intended to provide an ivy device, or the back of four other types of targets), which made it possible to greatly increase the It can also be effectively applied to a sputtering apparatus equipped with a magnetic field generating means.

すなわち、本発明は、ターゲットの背面IIに磁界発生
手段を設けたスパッタ装置において、′前記磁界発生手
段のターゲットに面する出接端物が高透磁率の軟磁性材
からなることを%像とするものである。
That is, the present invention provides a sputtering apparatus in which a magnetic field generating means is provided on the back surface II of the target, and that 'the welding end of the magnetic field generating means facing the target is made of a soft magnetic material with high magnetic permeability. It is something to do.

なお、上述の出接端部とは、磁界発生手段の実質的な磁
力線を発生する端部のことであり、磁界発生手段の磁界
発生源と一体であっても別体であっても良い。
Note that the above-mentioned contact end portion refers to an end portion of the magnetic field generating means that generates substantial lines of magnetic force, and may be integrated with or separate from the magnetic field generating source of the magnetic field generating means.

また、高透磁率の軟磁性材とは、通常のトランス等のコ
ア材と使用されるものならば通用でき、具体的には、軟
鋼、ケイ素鋼、パーマロイ郷が適用できるが、透磁率は
高い方が良く且つ飽和磁束密度が大きい材料が好ましい
In addition, soft magnetic materials with high magnetic permeability can be used as long as they are used as core materials for ordinary transformers, etc. Specifically, soft magnetic materials such as mild steel, silicon steel, and permalloy can be used, but they have high magnetic permeability. A material with a higher saturation magnetic flux density is preferable.

駅り本発明の詐細を前述の対向ターゲット式スパッタ装
置を例に図面に基いて説明する。
The advantages and disadvantages of the present invention will be explained with reference to the drawings, taking the above-mentioned facing target sputtering apparatus as an example.

第2図は本発明の前記実施例のト明図である。FIG. 2 is a schematic diagram of the embodiment of the present invention.

なお図の記号は、第1図と同じものには同じ記号を使用
しておる。
Note that the same symbols are used for the same parts as in FIG. 1.

図から明らかな通り、ターゲットT1 + ”2及び基
板20の真空槽10内の配置及びスパッタ電力の供給F
ii1図の従来の対向ターゲット式スバ。ツタi装置と
同じである。
As is clear from the figure, the arrangement of the target T1 + "2 and the substrate 20 in the vacuum chamber 10 and the supply of sputtering power F
ii The conventional facing target type suba shown in Figure 1. It is the same as the Tsuta i device.

しかし、ターゲットホルダー11.12#′i空胴榊造
とし冷却水の供給管17a、ljl&  及び排出管1
7b、18b  を設は冷却可能とし、絶縁部材15.
16を介して真空槽10に取着しである。なお、ターゲ
ットホルダー11.12はSUS材等の非磁性材からな
る。
However, the target holder 11.12#'i cavity Sakaki construction has cooling water supply pipe 17a, ljl & and discharge pipe 1.
7b and 18b can be cooled, and the insulating member 15.
It is attached to the vacuum chamber 10 via 16. Note that the target holders 11 and 12 are made of a non-magnetic material such as SUS material.

そして、磁界発生手段は、第1図の従来装置のコイル3
0に賛えて、以下のようになしである。すなわち、ター
ゲットホルダー11.12内のl−ゲ7 トT+ * 
Tm @ mにfi −ケア ) Tr * Ttの絢
辺に沿ってその背面にその先端面が対面するように配置
された先趨部が基端部より薄肉になさrlた硅素鋼等の
高透磁率軟磁性材からなるrm状枠体31.32と、筒
状枠体31.32の基端面に@着して配置された筒状枠
体31゜32と枠形がほぼ同じの筒状の永久磁石33゜
34とから構成すると共に、永久磁石33゜34の磁極
を図示の如く異極が対向するように配置した構成とし、
である。従って、永久磁石33.34を磁界発生源とし
、筒状枠体31゜32を磁極端部として、磁界Hけ図示
の如くターグツ)T、、T、ic垂直方向でその周辺部
のみに、ターグツ)T、、Ttの間の空間を囲繞する如
く簡 ・状に形成される。
The magnetic field generating means is the coil 3 of the conventional device shown in FIG.
In praise of 0, there is none as follows. That is, the l-gate 7 T+ * in the target holder 11.12
Tm @ m fi-care) Tr * Highly transparent material such as silicon steel whose distal end is thinner than its proximal end and is arranged along the fiber side of Tt so that its distal end face faces the back surface of Tt. An rm-shaped frame 31.32 made of a soft magnetic material, and a cylindrical frame 31.32 having almost the same frame shape as the cylindrical frame 31.32 disposed on the base end surface of the cylindrical frame 31. It is composed of permanent magnets 33° and 34, and the magnetic poles of the permanent magnets 33° and 34 are arranged so that different poles face each other as shown in the figure,
It is. Therefore, by using the permanent magnets 33, 34 as the magnetic field generation sources and the cylindrical frames 31 and 32 as the magnetic pole ends, the magnetic field H is generated only in the periphery in the vertical direction as shown in the figure. ) T, , Tt is formed in a simple shape surrounding the space between T, Tt.

以上のように構成しであるので、前述の従来の対向ター
ゲット式スパッタ装置と同じように、真空槽1G内を快
気系により排気口4oがら充分排気した債、ガス導入糸
から導入口50倉通してスパッタガスを導入し、シール
ドリンク13゜14とターゲットT、、T、にスパッタ
電源6oよリスバッタ電力を供給することKよりスパッ
タが行なわれ、基板2o上にターゲットT、、’r、i
c対応した博禮が形成される。
With the above configuration, in the same way as the conventional facing target type sputtering apparatus described above, the inside of the vacuum chamber 1G is sufficiently evacuated from the exhaust port 4o by the air system, and the gas introduction thread is passed through the inlet port 50. sputtering gas is introduced from K, and sputtering power is supplied from the sputtering power source 6o to the shield links 13 and 14 and the targets T, , T. Sputtering is performed from K, and the targets T, , 'r, i
c A corresponding Hakurei is formed.

ところで、前述の通り、磁界発生手段はターグツ)T1
.T、の後方のみに設けた構成のため、磁界はターゲッ
トT、、−関0みに限定されるが、適当な磁界であれば
、高エネルギーのγ電子等t−#!1図の従来装置と同
様にターグツ)T、、ち関に閉じ込めることができる。
By the way, as mentioned above, the magnetic field generating means is T1
.. Since the configuration is provided only behind the target T, the magnetic field is limited to the target T,, -, but if the magnetic field is suitable, high-energy γ electrons etc. t-#! Similar to the conventional device shown in Fig. 1, it is possible to confine the target to T, , , and .

従って、本構成においても、第1図の従来装置と同様罠
高速の1iI杉成ができる。
Therefore, with this configuration as well, high-speed 1iI signal formation can be achieved, similar to the conventional device shown in FIG.

このように1本発明によれば、第1図の従来の対向ター
ゲット式スパッタ装置の如く、外部コイルを設ける8賛
はなく、装置全体を小型化できる。これは装置が大型化
する工業規模の装fllにおいては非常に大きな効果と
なる。
As described above, according to the present invention, unlike the conventional facing target type sputtering apparatus shown in FIG. 1, there is no need to provide external coils, and the entire apparatus can be miniaturized. This is a very significant effect in industrial-scale installations where the equipment becomes larger.

父、磁界印加空間を必要最小限にして永久磁石の1史用
を口J能と1.たので、DL雑な電諒装置等が不要とな
り、装置全体の信頼性が向上すると共eこ全体として安
価な装置が可能となった・!e! llc s 磁界発
生手段として、筒状枠体の磁極南部と筒状の永久磁石を
ターゲットT1.T!の周辺部のみに設けた構成にする
ことKよりターゲットの冷却は、広い面積について一様
に効率よく行なうことが出来るので、スパッタ電力を増
して膜形成速度を増大させてもスパッタ向からのII!
l射熱を小さく抑えることができる。
My father, with J. No. 1, explained how to use permanent magnets by minimizing the magnetic field application space. This eliminates the need for complicated DL communication devices, improves the reliability of the entire device, and makes it possible to create an inexpensive device as a whole. e! llcs As a magnetic field generating means, the southern part of the magnetic pole of the cylindrical frame and the cylindrical permanent magnet are connected to the target T1. T! Since the target can be cooled uniformly and efficiently over a wide area, even if the sputtering power is increased and the film formation rate is increased, the II from the sputtering direction is !
l Heat radiation can be suppressed to a small level.

更に通属ターゲソF Tl + ”2の中氾・部が集中
的にスパッタされるのに対して、本発明による対向ター
ゲット式スパッタ4I&eではターゲツト面が一様にス
パッタされる効果が得られた。
Furthermore, whereas the common target sputter FTl+''2 sputters intensively in the middle part, the opposed target sputter 4I&e according to the present invention has the effect that the target surface is sputtered uniformly.

かかる効果が得られる塩山は次のように考えられる。す
なわち、実施例に示す如く、磁極端部となる筒状枠体3
1.32をターゲット丁h1の周辺部に設けることによ
p、前述の通り、筒状の磁界が形成され、磁界のI!を
ターゲット”S 、1%の周辺空間に形成することにな
る。このためプラズマ中の高エネルギー電子やイオンは
磁界の壁によってターグツF ”1 a ”を間の空間
内にほとんど閉じ込められるが、ターゲットT11−の
周辺部以外では磁界が弱いので電子やイオンの飛行過板
を拘束しなくなる。従って、ターゲット表面近傍の電界
で附勢された電子はターゲットTI a Tmの広い領
域を飛行することによって、スパッタガスイオンの密度
分布をターゲットT1.TIの広い面積内に均一化する
。このスパッタガスイオンか均一に分布することによっ
てターゲツト面が一株にスパッタされる効果が得られる
と考えられる。
Salt mountains that can achieve this effect can be thought of as follows. That is, as shown in the embodiment, the cylindrical frame 3 that becomes the magnetic pole tip
By providing 1.32 at the periphery of the target h1, a cylindrical magnetic field is formed as described above, and the magnetic field I! is formed in the space surrounding the target "S", 1% of the target.For this reason, high-energy electrons and ions in the plasma are mostly confined within the space between the target "S" and the target "1 a" by the magnetic field wall. Since the magnetic field is weak in areas other than the periphery of T11-, it does not restrict the flight plate of electrons and ions. Therefore, the electrons energized by the electric field near the target surface fly over a wide area of the target TI a Tm. The density distribution of the sputtering gas ions is made uniform within a wide area of the target T1.TI.It is thought that by uniformly distributing the sputtering gas ions, an effect is obtained in which the target surface is sputtered all at once.

また、磁界発生手段を、ターゲラ)TI、T、の鳩辺部
に沿って配置した、磁極端部となる為透磁4=1#磁性
材からなる筒状枠体3]、32とその&烟11に密着し
た筒状の永久磁石38.34とで構成したので、以下の
通抄、謝に優れたスパッタ幼果が得られる。
In addition, the magnetic field generating means is arranged along the pigtail part of the tagera) TI, T, and the cylindrical frame body 3], 32 made of magnetic material and its & Since it is composed of the cylindrical permanent magnets 38 and 34 that are in close contact with the smoke 11, it is possible to obtain sputtered seedlings that are excellent in the following properties.

すなわち、高透磁率軟磁性部材からなる磁極錫部會介し
て、磁界はその%Qsを磁極として間M的に果申して形
成できるので、mumsの先端部の配置により磁界の壁
のターゲラ) T、 、 T!との位置関係を#J4!
Ilでき、その外周縁部のみにも%生でき乙。促って、
γ電子を強く抑制する愉域は、i慣端部となる(資)状
忰体を設けない水久員石のみの場合と比較して婆らにタ
ーゲット外周縁部のみに限定でき、スパッタガスイオン
の踏戻分布をターゲットTl a T2の広い面積に拡
大することができる。
That is, the magnetic field can be formed by exerting the %Qs as a magnetic pole through the magnetic pole tin part made of a high magnetic permeability soft magnetic material, so depending on the arrangement of the tip of the mums, the target area of the wall of the magnetic field (T) , , T! Positional relationship with #J4!
It is possible to grow only on the outer periphery. Urge me,
Compared to the case of only Mizukumenite, which does not have a (material)-shaped structure that serves as the i-conducting edge, the region where γ electrons can be strongly suppressed can be limited to only the outer periphery of the target, and the sputter gas The return distribution of ions can be expanded over a wide area of the target Tla T2.

また、?MJ透磁率軟磁性部材の磁極端部を介在させろ
ことにより、永久磁石の反磁界が減少し、ターゲット外
周縁部に形成される磁界を強めるので、対面するターゲ
ットの面間隔を広げてスパッタが可*I−になる。
Also,? By interposing the magnetic pole end of the MJ magnetic permeability soft magnetic member, the demagnetizing field of the permanent magnet is reduced and the magnetic field formed at the outer periphery of the target is strengthened, so sputtering can be performed by widening the distance between the faces of the facing targets. *Becomes I-.

史に、高透磁率軟磁性部材の磁極端部の介在により永久
磁石から一様な磁界がターゲラ) T1゜T、の外縁部
に形成さられるのでγ電子を抑制する領域は一様になる
ため、ターゲットの侵食領域の一#恨が増大する。
Historically, due to the presence of the magnetic pole tip of a high magnetic permeability soft magnetic member, a uniform magnetic field from the permanent magnet is formed at the outer edge of T1゜T, so the area where γ electrons are suppressed becomes uniform. , the number of grudges in the target's eroded area increases.

筐次、磁極端部の筒状枠体の形状寸法をターゲットTI
、TIの背面に面する先端側が薄肉となるようにするこ
とによりターゲットの冷却能力を増すことがさらに容易
となる。
Tsuyoshi, target TI of the shape and dimensions of the cylindrical frame of the magnetic pole tip.
By making the tip side facing the back side of the TI thinner, it becomes easier to increase the cooling capacity of the target.

また、磁極端部を別体の筒状枠体とし磁力線はその先端
部から生ずる構成のため、磁界発生源となる永久磁石3
3.34の形状寸法及び配置はターゲットボルダ−内に
組込めれば良いので、永久磁石33.34の製作が容易
となり、スパッタ装置が安価となる。
In addition, since the magnetic field end is a separate cylindrical frame and the lines of magnetic force are generated from the tip, the permanent magnet 3 which becomes the magnetic field generation source
Since the dimensions and arrangement of the permanent magnets 33 and 34 only need to be incorporated into the target boulder, the permanent magnets 33 and 34 can be manufactured easily and the sputtering apparatus can be made inexpensive.

以上、本発明を実施例に基いて説明したが、本発明はか
かる実施例KII[I定されるものでない。
Although the present invention has been described above based on Examples, the present invention is not limited to such Examples KII.

対向ターゲット式スパッタ装置を例に説明し。This will be explained using a facing target sputtering device as an example.

たが、ターゲットの背面側に磁界焉生手IIiを配置し
てターゲット前面側に磁界を形成させるようKしたスパ
ッタ装置、例えはマグネトロン式スパッタ装置にも効果
的−適用できる。
However, the present invention can also be effectively applied to a sputtering apparatus, for example, a magnetron type sputtering apparatus, in which the magnetic field generator IIi is arranged on the back side of the target to form a magnetic field on the front side of the target.

また磁Ik遍部を先端部が基端部より薄肉となったim
m面が楔状の筒状枠体となしたものを示したが、その形
状は磁界発生源からの磁束を効果的に先端部から細巾の
磁界を形成するように尋〈ものであれは良く、従ってそ
のIll断面が先細となるものであれば良い。
In addition, the tip of the magnetic Ik is thinner than the base.
The m-plane has a wedge-shaped cylindrical frame, but its shape is designed to effectively channel the magnetic flux from the magnetic field source to form a narrow magnetic field from the tip. , Therefore, it is sufficient if its Ill cross section is tapered.

更に、4Iay1−%生手段はターゲットホルダー内に
収納したものを示したが、ターゲット部の構成により適
宜設計すべきであり、ターゲットホルタ−の外周に設け
ても良いことは云うまでもない。
Furthermore, although the 4Iay1-% production means is shown as being housed in the target holder, it should be designed appropriately depending on the configuration of the target portion, and it goes without saying that it may be provided on the outer periphery of the target holder.

μ)上の通り、本発明は、γ電子等のスパッタ粒子をa
I促しプラズマ密度を高める磁界をターゲット前面側に
形成する磁界発生手段の効率向上に寄与するところ大の
ものであり、かかる磁界発生手段を備えたスパッタ装置
の性能向上に非常に大きな効果を奏するものである。
μ) As mentioned above, the present invention allows sputtered particles such as γ electrons to be
This greatly contributes to improving the efficiency of the magnetic field generating means that creates a magnetic field on the front side of the target that increases the plasma density by increasing plasma density, and has a very large effect on improving the performance of sputtering equipment equipped with such a magnetic field generating means. It is.

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

1g1図は従来f・対向ターゲット式スパッタ装置の説
明図、第2図は本発明に係わる対向ターゲット式スパッ
タ装置の鰭明図である。 ”l * Tlけターゲット、10は真空橿−,2Gは
基板、31.32は筒状枠体、33.3’4は永久磁石
。 第1困 オこ図
1g1 is an explanatory diagram of a conventional f. facing target type sputtering apparatus, and FIG. 2 is a fin view of the facing target type sputtering apparatus according to the present invention. 10 is a vacuum rod, 2G is a substrate, 31.32 is a cylindrical frame, and 33.3'4 is a permanent magnet. 1st diagram

Claims (1)

【特許請求の範囲】 1、 ターゲットの背面@に磁界発生手段を設けたスパ
ッタ装置において、前記磁界発生手段のターゲットに面
する磁極端部が高透磁率の歌磁性材からなること1r−
4?徴とするスパクタ襲!。 λ 前記a礪7IA部の側断面が先細形状である特許請
求の範囲第1よ記載のスパッタ装置−1前記ターゲット
が互いに平行に対面した対向ターゲットであり、その各
々のターゲットの前記a糎211部をターゲットの周辺
に沿つ之筒状砕体となし念特許請求の範囲第1項若しく
Fi第2導記載のスパッタ装置。 4、 前記磁界発生手段が前記磁駕端邪の筒状枠体とそ
の背後に同心的に配置したm−惨状の永7磁石とからな
る特許請求の範囲I!3項記塁のスパッタ鉄性。 5 @記磁極端部の葡状枠体の先端部を基部より薄肉と
しft特許請求の範囲第4墳耐“載(rrスパッタ装置
[Scope of Claims] 1. In a sputtering apparatus in which a magnetic field generating means is provided on the back side of a target, a magnetic field end portion of the magnetic field generating means facing the target is made of a magnetic material with high magnetic permeability.
4? A sign of a spacta attack! . λ A sputtering apparatus according to claim 1, wherein the side cross section of the a-glue 7IA section is tapered. The sputtering apparatus according to claim 1 or Fi 2, wherein the cylindrical crushing body is formed along the periphery of the target. 4. Claim I! wherein the magnetic field generating means comprises the cylindrical frame of the magnetic field and an m-shaped magnet disposed concentrically behind the cylindrical frame. Sputtered iron as described in Section 3. 5 @ The tip of the grape-shaped frame at the magnetic pole end is made thinner than the base.
JP7024582A 1982-04-28 1982-04-28 Sputtering device Granted JPS58189370A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7024582A JPS58189370A (en) 1982-04-28 1982-04-28 Sputtering device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7024582A JPS58189370A (en) 1982-04-28 1982-04-28 Sputtering device

Publications (2)

Publication Number Publication Date
JPS58189370A true JPS58189370A (en) 1983-11-05
JPS6343465B2 JPS6343465B2 (en) 1988-08-30

Family

ID=13425982

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7024582A Granted JPS58189370A (en) 1982-04-28 1982-04-28 Sputtering device

Country Status (1)

Country Link
JP (1) JPS58189370A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103014632A (en) * 2011-09-26 2013-04-03 中国科学院金属研究所 Arc ion iron plating magnetic composite structural target and application thereof

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5347384A (en) * 1976-10-13 1978-04-27 Nec Corp Sputtering apparatus

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5347384A (en) * 1976-10-13 1978-04-27 Nec Corp Sputtering apparatus

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103014632A (en) * 2011-09-26 2013-04-03 中国科学院金属研究所 Arc ion iron plating magnetic composite structural target and application thereof
CN103014632B (en) * 2011-09-26 2015-12-09 中国科学院金属研究所 A kind of arc ion plating ferromagnetic composite structure target material and application thereof

Also Published As

Publication number Publication date
JPS6343465B2 (en) 1988-08-30

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