JPH07166346A - Magnetron sputtering device - Google Patents
Magnetron sputtering deviceInfo
- Publication number
- JPH07166346A JPH07166346A JP31213393A JP31213393A JPH07166346A JP H07166346 A JPH07166346 A JP H07166346A JP 31213393 A JP31213393 A JP 31213393A JP 31213393 A JP31213393 A JP 31213393A JP H07166346 A JPH07166346 A JP H07166346A
- Authority
- JP
- Japan
- Prior art keywords
- target
- permanent magnets
- magnetic field
- substrate
- magnetron sputtering
- 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.)
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- Physical Vapour Deposition (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、主として半導体や電子
機器の製造工程で基板上に薄膜を形成するために使用さ
れるマグネトロンスパッタリング装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetron sputtering apparatus mainly used for forming a thin film on a substrate in a semiconductor or electronic device manufacturing process.
【0002】[0002]
【従来の技術】半導体や電子機器の製造工程に於いて、
薄膜を基板上に形成する場合、取扱いの容易さや制御性
の良さからマグネトロンスパッタリング法が多く利用さ
れている。これに使用されている装置の概略は図1に示
す如くであり、真空槽a内に基板bと成膜させたい物質
の円形や長方形のターゲットcとを対向させて配置し、
該真空槽a内にはAr等の放電ガスを放電ガス導入口i
から導入すると共に該真空槽a内を真空排気口jから排
気して一定の減圧状態に維持し、ターゲットc側に負電
圧を印加して放電を起こさせる。この放電により発生し
たガス分子(イオン)が負電圧で加速されてターゲット
cに入射し、ターゲット表面の原子を叩き出し、余弦法
則によって四方へ飛出していく原子の一部が基板b上に
堆積して薄膜を形成する。hはターゲット電極、kは直
流電源、lは基板ホルダ、mは磁力線を示す。該ターゲ
ットcの背後には磁石dを配し、これでターゲットcの
前方に電子を拘束する磁場を形成してマグネトロン放電
を発生させ、成膜速度を高めている。磁石dとしては、
永久磁石或は電磁石が用いられるが、ターゲット表面で
の磁場のターゲット表面に対する垂直成分が0になる位
置(図中A点)が最も放電の効率が高く、A点の周辺の
ターゲットが最も多くスパッタされる。通常、この部分
はエロージョン領域と呼ばれている。この部分で、電子
はE×Bドリフトを行ないながら徐々に電離が進んでい
く。磁場は閉ループになるように作らないと、エロージ
ョン領域でイオンの密度分布差が生じてしまう。開ルー
プの磁場を作ると、閉ループの場合に比べて低い圧力で
放電が起こりにくいという結果になる。2. Description of the Related Art In the manufacturing process of semiconductors and electronic devices,
When forming a thin film on a substrate, the magnetron sputtering method is often used because of its easy handling and good controllability. An outline of an apparatus used for this is as shown in FIG. 1, in which a substrate b and a circular or rectangular target c of a substance to be formed are arranged in a vacuum chamber a so as to face each other.
A discharge gas such as Ar is supplied into the vacuum chamber a through a discharge gas inlet i.
In addition, the inside of the vacuum chamber a is evacuated from the vacuum exhaust port j to maintain a constant depressurized state, and a negative voltage is applied to the target c side to cause discharge. Gas molecules (ions) generated by this discharge are accelerated by a negative voltage and are incident on the target c, knocking out atoms on the target surface, and some of the atoms that fly out in all directions by the cosine law are deposited on the substrate b. To form a thin film. h is a target electrode, k is a DC power supply, l is a substrate holder, and m is a magnetic field line. A magnet d is arranged behind the target c, and a magnetic field for confining electrons is formed in front of the target c to generate magnetron discharge, thereby increasing the film formation rate. As the magnet d,
A permanent magnet or electromagnet is used, but the discharge efficiency is highest at the position where the vertical component of the magnetic field on the target surface is 0 (point A in the figure), and the target around point A is the most sputter. To be done. This part is usually called an erosion area. In this portion, the electrons gradually ionize while making an E × B drift. Unless the magnetic field is made so as to form a closed loop, a difference in ion density distribution will occur in the erosion region. Creating an open loop magnetic field results in less discharge at lower pressures than in the closed loop case.
【0003】磁石dとして電磁石を用いた電磁石カソー
ドでは、磁場を発生させるコイルを2重或は3重とし、
夫々のコイルに流す電流の向きや大きさを制御してエロ
ージョン領域の位置や面積を変えることができる。その
ため、ターゲットcの表面全域をスパッタすることが可
能である。また、電流の制御を最適化することにより、
基板に形成される膜厚を均一化することができる。In an electromagnet cathode using an electromagnet as the magnet d, the coil for generating a magnetic field is double or triple,
The position and area of the erosion region can be changed by controlling the direction and magnitude of the current flowing through each coil. Therefore, it is possible to sputter the entire surface of the target c. Also, by optimizing the current control,
The film thickness formed on the substrate can be made uniform.
【0004】磁石dに永久磁石を用いると、上記の電磁
石のような制御ができないため、図2、図3の断面図に
示すように、永久磁石を動かすことにより同様な効果が
得られるようにしている。図2は永久磁石を扇形のエロ
ージョン領域が得られるように扇形部を有する内側磁石
eと外側磁石fを組んだもので、扇形部の円弧の中心を
回転中心gとしてターゲット電極hに対して回転させる
ことにより、扇形のエロージョン領域がターゲットcの
表面全面を移動し、表面全域がスパッタされる。該扇形
部の中心角(円弧の長さ)を調整することにより、膜厚
分布の調整ができる。図3の場合は、円環状の内側磁石
nと外側磁石oとを組み、これをターゲット電極hに対
し偏心回転させることで環状のエロージョン領域がター
ゲットcの表面全面を移動し、表面全域がスパッタされ
る。偏心量を変えると、わずかではあるが、膜厚分布の
調整も行なえる。When a permanent magnet is used as the magnet d, it cannot be controlled like the above electromagnet. Therefore, as shown in the sectional views of FIGS. 2 and 3, by moving the permanent magnet, the same effect can be obtained. ing. FIG. 2 shows a permanent magnet in which an inner magnet e having a fan-shaped portion and an outer magnet f are assembled so that a fan-shaped erosion region is obtained. The permanent magnet is rotated with respect to a target electrode h with a center of an arc of the fan-shaped portion as a rotation center g. By doing so, the fan-shaped erosion region moves over the entire surface of the target c, and the entire surface is sputtered. The film thickness distribution can be adjusted by adjusting the central angle (arc length) of the fan-shaped portion. In the case of FIG. 3, an annular inner magnet n and an outer magnet o are assembled and eccentrically rotated with respect to the target electrode h so that the annular erosion region moves over the entire surface of the target c and the entire surface is sputtered. To be done. By changing the amount of eccentricity, the film thickness distribution can be adjusted, albeit slightly.
【0005】[0005]
【発明が解決しようとする課題】磁石dが電磁石である
と、これの電流量や電流方向を変えるだけでハードウエ
アの変更なしに様々な径のエロージョン領域を形成でき
ることが最大のメリットであるが、電磁石を回転させる
ことが難しくターゲットcの中心部分がスパッタされな
いという欠点がある。このようなスパッタされない部分
には、エロージョン領域でスパッタされた原子が堆積
し、これが剥がれ落ちてダストとなり、膜質を低下させ
てしまうので好ましくない。また、電磁石は、強い磁界
を発生させるために大きなコイルを必要とし、体積、質
量とも永久磁石に比べて大きくなる。さらに、電流の制
御回路が必要でコストの面でも高くなる。When the magnet d is an electromagnet, the greatest merit is that it is possible to form erosion regions of various diameters by changing the current amount and the current direction of the magnet d without changing the hardware. However, there is a drawback that it is difficult to rotate the electromagnet and the central portion of the target c is not sputtered. Atoms sputtered in the erosion region are deposited on such a portion that is not sputtered, and this is peeled off to become dust, which is not preferable because it deteriorates the film quality. In addition, the electromagnet requires a large coil to generate a strong magnetic field, and has a larger volume and mass than the permanent magnet. In addition, a current control circuit is required, which increases the cost.
【0006】磁石dが永久磁石の場合は、電磁石のよう
な問題はないが、エロージョン領域の径を変更するには
ハードウエアの変更が必要である。例えば、図2の場
合、膜厚分布を制御するためには扇形の角度(円弧の長
さ)を調整する必要があり、最適な膜厚分布を得るため
に幾つかの磁石を作って実験しなければならず、これは
手間とコストがかかりすぎて好ましくない。また、図3
の場合、磁石dを固定して放電させるとターゲットcの
表面には円形のエロージョン領域が形成され、該磁石を
偏心回転させることによって、ターゲット表面でのエロ
ージョン領域の滞在時間から、同心円状の2つのエロー
ジョン領域が出来上がる。この場合のターゲットcの断
面形状は図4に示す如くであり、内側のエロージョン領
域と外側のエロージョン領域のスパッタ量はほぼ同じと
なり、そのため膜厚分布は基板の中央付近が厚く、周辺
部にいくほど薄くなる。分布の調整は磁石の偏心量の変
更によってもできるが、わずかな調整しかできず、基本
的には磁石の径を変えなくてはならないのでその調整は
簡単でない。When the magnet d is a permanent magnet, there is no problem like an electromagnet, but hardware must be changed to change the diameter of the erosion region. For example, in the case of FIG. 2, it is necessary to adjust the fan-shaped angle (the length of the arc) in order to control the film thickness distribution, and several magnets were made to perform an experiment in order to obtain the optimum film thickness distribution. This is not preferable because it requires too much labor and cost. Also, FIG.
In this case, when the magnet d is fixed and discharged, a circular erosion region is formed on the surface of the target c, and by rotating the magnet eccentrically, it is possible to determine the concentric circular erosion region from the residence time of the erosion region on the target surface. Two erosion areas are completed. The cross-sectional shape of the target c in this case is as shown in FIG. 4, and the sputter amounts of the inner erosion region and the outer erosion region are almost the same, so that the film thickness distribution is thick near the center of the substrate and goes to the peripheral portion. The thinner it gets. The distribution can be adjusted by changing the amount of eccentricity of the magnet, but only a slight adjustment can be made, and basically the diameter of the magnet must be changed, so that adjustment is not easy.
【0007】本発明は、磁石を変更することなく膜厚分
布の充分な調整を行なえ、しかもターゲットの全面をス
パッタできる永久磁石を使用したマグネトロンスパッタ
リング装置を提供することを目的とするものである。An object of the present invention is to provide a magnetron sputtering apparatus using a permanent magnet capable of sufficiently adjusting the film thickness distribution without changing the magnet and capable of sputtering the entire surface of the target.
【0008】[0008]
【課題を解決するための手段】本発明では、基板と対向
してターゲットを設け、該ターゲットの背後にこれに沿
って回転する複数個の永久磁石を設けて該ターゲットの
前方に閉ループの磁界を形成するマグネトロンスパッタ
リング装置に於いて、該複数個の永久磁石を、そのター
ゲットの背面の中心部寄りと対向する側において該背面
に対して接近離反自在に設けることにより、上記の目的
を達成するようにした。また、上記の目的の一部は、該
複数個の永久磁石とターゲットとの間に部分的に磁性体
を介在させて該ターゲットの表面の磁界強度を部分的に
弱めることによっても達成できる。According to the present invention, a target is provided facing a substrate, and a plurality of permanent magnets rotating along the target are provided behind the target to generate a closed loop magnetic field in front of the target. In a magnetron sputtering device to be formed, the above-mentioned object is achieved by providing the plurality of permanent magnets so that the permanent magnets can be moved toward and away from the back surface of the target on the side facing the central portion of the back surface. I chose Part of the above object can also be achieved by partially interposing a magnetic material between the plurality of permanent magnets and the target to partially weaken the magnetic field strength on the surface of the target.
【0009】[0009]
【作用】通常のスパッタリングと同様に真空槽内に放電
ガスを導入して減圧状態を維持し、ターゲット電極に負
電圧を印加すると、ターゲットの背後で回転する永久磁
石の磁界の作用によりマグネトロン放電が発生するが、
該永久磁石のターゲットの背面の中心部寄りと対向する
側を該背面に対して接近離反させて該永久磁石を傾斜さ
せることにより、或は該永久磁石とターゲットの間に介
在する磁性体の厚さを変更することにより、ターゲット
表面の内側と外側で有効磁界を変えてイオンの分布を変
えることができ、スパッタ量はイオン量に比例するので
エロージョン領域を変更して永久磁石では通常はスパッ
タされにくいターゲットの中心部をスパッタすることが
でき、かくて、ターゲット全面をスパッタすると共に膜
厚分布の自在な調整を行なえる。[Operation] Similar to normal sputtering, when a discharge gas is introduced into the vacuum chamber to maintain a reduced pressure and a negative voltage is applied to the target electrode, the magnetic field of the permanent magnet rotating behind the target causes magnetron discharge. Occurs,
The thickness of the magnetic body interposed between the permanent magnet and the target by tilting the permanent magnet by moving the side of the permanent magnet facing the center of the back surface of the target closer to or away from the back surface. By changing the depth, it is possible to change the effective magnetic field inside and outside the target surface to change the ion distribution.Since the amount of spatter is proportional to the amount of ion, the erosion area is changed to sputter normally. It is possible to sputter the central part of the target, which is difficult to sputter, and thus to sputter the entire surface of the target and freely adjust the film thickness distribution.
【0010】[0010]
【実施例】本発明の実施例を図面に基づき説明すると、
図5に於いて、符号1は真空ポンプに接続される真空排
気口2とArガス等の放電ガスを導入する導入口3とを
備えた真空槽を示し、該真空槽1の内部には、基板ホル
ダ4に支持されたシリコンウエハ等の基板5と成膜させ
たい物質から成る円形や長方形のターゲット6とが対向
して配置される。該ターゲット6は直流電源18或は高
周波電源に接続されたターゲット電極7上に固定され
る。該ターゲット6の背後にはベース9に取付けた複数
個の永久磁石8が該ターゲット6に沿って回転自在に設
けられ、該ターゲット6の表面を巡る閉ループの磁界1
6を形成する。この永久磁石8は、図6に示す如く、円
板状の内側磁石8aとこれを等間隔の間隔10を存して
囲む円環状の外側磁石8bの2個で構成し、その中心を
ターゲット6の中心11に対して偏心させ、該中心11
を中心に回転されるようにした。該永久磁石8は大小の
環状の3個以上を使用して3重以上の円環状に構成する
ことも可能であり、内側磁石8aは環状に構成すること
も可能である。Embodiments of the present invention will be described with reference to the drawings.
In FIG. 5, reference numeral 1 denotes a vacuum chamber provided with a vacuum exhaust port 2 connected to a vacuum pump and an inlet port 3 for introducing a discharge gas such as Ar gas. Inside the vacuum chamber 1, A substrate 5 such as a silicon wafer supported by a substrate holder 4 and a circular or rectangular target 6 made of a substance to be deposited are arranged to face each other. The target 6 is fixed on a target electrode 7 connected to a DC power supply 18 or a high frequency power supply. Behind the target 6, a plurality of permanent magnets 8 mounted on a base 9 are rotatably provided along the target 6, and a closed loop magnetic field 1 around the surface of the target 6 is provided.
6 is formed. As shown in FIG. 6, the permanent magnet 8 is composed of a disk-shaped inner magnet 8a and an annular outer magnet 8b that surrounds the disk-shaped inner magnet 8a at regular intervals 10 and the center of the magnet 6 is the target 6. Eccentric to the center 11 of the
It was made to rotate around. The permanent magnet 8 can be formed in a triple or more annular shape by using three or more large and small annular shapes, and the inner magnet 8a can also be formed in an annular shape.
【0011】こうした構成では、永久磁石8が回転され
ても磁界の分布を変更しての膜厚調整も困難であるが、
本発明では、該永久磁石8の該ターゲット6の背面の中
心部寄りと対向する側を、該背面に対して接近離反自在
に設けることにより、該永久磁石8を傾斜させ、該ター
ゲット6の全面のスパッタと基板5に形成される膜厚の
調整を行なうようにした。これを更に説明すると、該永
久磁石8の全体の径を該ターゲット6の径の1/2以上
の大きさとし、該永久磁石8を、例えば図7に示すよう
に、該ターゲット電極7の背後に設けた該ターゲット6
の中心11と一致してモータ15で回転される円板状の
回転ステージ12に支持部材13、14で支持するよう
にした。これら支持部材13、14は揺動自在に永久磁
石8を支持し、ターゲット6の中心11寄りの支持部材
14をシリンダやモータ、或はねじ等の適当な手段によ
り昇降させると、ターゲット6の背面に対して永久磁石
8が接近離反し、該ターゲット6の表面の磁界分布が可
変される。即ち、支持部材14を図面で上方へ引き上げ
ると、ターゲット6の表面の磁界は、その中心部分が周
辺部分に比べて弱くなり、該中心部分のイオン密度が該
周辺部分よりも弱められることによって基板5の中心部
分に堆積する膜厚を減少できる。通常は基板5の中心部
分の膜厚がその周辺部分よりも厚くなりがちであるが、
永久磁石8をターゲット6より離反させ回転させること
により磁石の設計を変更することなく膜厚の均一化を図
れる。また、永久磁石8の傾斜によりターゲット6の表
面の磁界が相対的に移動し、これに伴ってスパッタ領域
が移動するので、ターゲット6の全面に亘るスパッタを
行なえる。With such a structure, it is difficult to adjust the film thickness by changing the distribution of the magnetic field even if the permanent magnet 8 is rotated.
In the present invention, the side of the permanent magnet 8 facing the central portion of the back surface of the target 6 is provided so as to be able to move toward and away from the back surface so that the permanent magnet 8 is tilted and the entire surface of the target 6 is tilted. And the film thickness formed on the substrate 5 was adjusted. To further explain this, the entire diameter of the permanent magnet 8 is set to 1/2 or more of the diameter of the target 6, and the permanent magnet 8 is placed behind the target electrode 7 as shown in FIG. 7, for example. The target 6 provided
The supporting members 13 and 14 support the disk-shaped rotary stage 12 which is rotated by the motor 15 so as to coincide with the center 11 of the. These support members 13 and 14 swingably support the permanent magnet 8, and when the support member 14 near the center 11 of the target 6 is lifted and lowered by an appropriate means such as a cylinder, a motor, or a screw, the back surface of the target 6 is reached. In contrast, the permanent magnet 8 approaches and separates, and the magnetic field distribution on the surface of the target 6 is changed. That is, when the support member 14 is pulled upward in the drawing, the magnetic field on the surface of the target 6 becomes weaker in the central portion than in the peripheral portion, and the ion density in the central portion is weakened than in the peripheral portion, so that the substrate It is possible to reduce the film thickness deposited in the central portion of No. 5. Normally, the thickness of the central portion of the substrate 5 tends to be thicker than that of the peripheral portion,
By rotating the permanent magnet 8 away from the target 6 and rotating it, the film thickness can be made uniform without changing the design of the magnet. Further, since the magnetic field on the surface of the target 6 relatively moves due to the inclination of the permanent magnet 8, and the sputtering region moves accordingly, it is possible to perform sputtering over the entire surface of the target 6.
【0012】該永久磁石8とターゲット6との間に、図
8、図9に示すように、部分的に磁性体17を介在させ
ることによっても、本発明の膜厚分布の調整の目的は達
成できる。この場合、ターゲット6の中心11付近と対
応する永久磁石8の表面に扇形の鉄製その他の磁性体1
7を取付けたもので、該磁性体17により該永久磁石8
からターゲット6の表面へ漏れる磁界が弱められ、該永
久磁石8をターゲット6の中心11を中心として回転さ
せると、上記のように永久磁石8を傾けたときと同様
に、ターゲット6の中心部分の磁界がその周辺部分の磁
界よりも弱いため、該中心部分のイオン密度が該周辺部
分よりも弱められ、基板5の中心部分に堆積する膜厚を
永久磁石8の設計を変更せずに減少させ得る。尚、該永
久磁石8の構成は図6のものと変わりがない。該磁性体
17は、図10のように、環状の永久磁石8の中心部分
に対応する部分が薄く、周辺部分に対応する部分に至る
につれ厚くなるテーパ状のものを使用してもよく、この
場合は、ターゲット6の表面の磁界の強度分布をその周
辺から中心に向かって逓減させることができる。ところ
で、上記実施例では永久磁石8の表面に磁性体17を取
付けているが、これはターゲット電極7の背面に取付け
てもよい。The objective of adjusting the film thickness distribution of the present invention can be achieved also by partially interposing a magnetic material 17 between the permanent magnet 8 and the target 6 as shown in FIGS. it can. In this case, a fan-shaped iron or other magnetic body 1 is formed on the surface of the permanent magnet 8 corresponding to the vicinity of the center 11 of the target 6.
7 is attached to the permanent magnet 8 by the magnetic body 17.
The magnetic field leaking from the target to the surface of the target 6 is weakened, and when the permanent magnet 8 is rotated about the center 11 of the target 6, the center portion of the target 6 is rotated in the same manner as when the permanent magnet 8 is tilted as described above. Since the magnetic field is weaker than that of the peripheral portion, the ion density of the central portion is weakened as compared with the peripheral portion, and the film thickness deposited on the central portion of the substrate 5 is reduced without changing the design of the permanent magnet 8. obtain. The structure of the permanent magnet 8 is the same as that shown in FIG. As shown in FIG. 10, the magnetic body 17 may be of a tapered shape in which the portion corresponding to the central portion of the annular permanent magnet 8 is thin and the thickness thereof increases toward the portion corresponding to the peripheral portion. In this case, the intensity distribution of the magnetic field on the surface of the target 6 can be gradually reduced from its periphery to its center. By the way, in the above embodiment, the magnetic body 17 is attached to the surface of the permanent magnet 8, but it may be attached to the back surface of the target electrode 7.
【0013】[0013]
【発明の効果】以上のように本発明によるときは、マグ
ネトロンスパッタリング装置のターゲットの背後で回転
する複数個の永久磁石を、そのターゲットの背面の中心
部付近と対向する側において該背面に対して接近離反自
在に設けたので、ターゲットの中心部分の磁界を弱めて
自在に膜厚分布を調整することができ、永久磁石の設計
を変更する必要もなく接近離反させる構成も簡単で比較
的安価に製作できる等の効果があり、また、該複数個の
永久磁石とターゲットとの間に部分的に磁性体を介在さ
せて該ターゲットの表面の磁界強度を部分的に弱めるこ
とによっても前記と同様の効果が得られる。As described above, according to the present invention, a plurality of permanent magnets rotating behind the target of the magnetron sputtering apparatus are provided on the back surface of the target on the side facing the central portion of the back surface. Since it is provided so that it can approach and separate freely, the magnetic field at the center of the target can be weakened to freely adjust the film thickness distribution, and the structure for approaching and separating without the need to change the design of the permanent magnet is simple and relatively inexpensive. There is an effect that it can be manufactured, and also by partially interposing a magnetic material between the plurality of permanent magnets and the target to partially weaken the magnetic field strength of the surface of the target, the same as the above. The effect is obtained.
【図1】 従来例の截断側面図FIG. 1 is a cutaway side view of a conventional example.
【図2】 従来の永久磁石の平面図FIG. 2 is a plan view of a conventional permanent magnet.
【図3】 他の従来の永久磁石の平面図FIG. 3 is a plan view of another conventional permanent magnet.
【図4】 図3の場合のターゲットの消耗状態の説明図FIG. 4 is an explanatory view of the consumption state of the target in the case of FIG.
【図5】 本発明の実施例の截断側面図FIG. 5 is a cutaway side view of the embodiment of the present invention.
【図6】 図5の6−6部分の平面図6 is a plan view of a portion 6-6 in FIG.
【図7】 本発明の具体的実施例の要部の側面図FIG. 7 is a side view of an essential part of a specific embodiment of the present invention.
【図8】 請求項3に記載の発明の実施例の要部の側面
図FIG. 8 is a side view of an essential part of the embodiment of the invention described in claim 3;
【図9】 図8の平面図9 is a plan view of FIG.
【図10】 請求項3に記載の発明の他の実施例の要部
の側面図FIG. 10 is a side view of the essential parts of another embodiment of the invention as set forth in claim 3;
1 真空槽 5 基板
6 ターゲット 8、8a、8b 永久磁石 11 中心 1
2 回転ステージ 16 磁界 17 磁性体1 vacuum tank 5 substrate
6 Target 8, 8a, 8b Permanent magnet 11 Center 1
2 rotating stage 16 magnetic field 17 magnetic material
Claims (3)
ーゲットの背後にこれに沿って回転する複数個の永久磁
石を設けて該ターゲットの前方に閉ループの磁界を形成
するマグネトロンスパッタリング装置に於いて、該複数
個の永久磁石を、そのターゲットの背面の中心部付近と
対向する側において該背面に対して接近離反自在に設け
たことを特徴とするマグネトロンスパッタリング装置。1. A magnetron sputtering apparatus in which a target is provided facing a substrate, and a plurality of permanent magnets rotating along the target are provided behind the target to form a closed loop magnetic field in front of the target. A magnetron sputtering apparatus, wherein the plurality of permanent magnets are provided so as to be able to move toward and away from the back surface of the target on the side facing the vicinity of the center of the back surface of the target.
ーゲットの背面に沿って回転自在に回転ステージを設
け、これに該回転ステージの回転中心から偏心させて該
ターゲットの直径の1/2以上の径の同心円状に配置し
た複数個の永久磁石を取付け、上記複数個の該永久磁石
を、そのターゲットの背面の中心部付近と対向する側に
おいて該背面に対して接近離反自在となるように該回転
ステージに取付けたことを特徴とする請求項1に記載の
マグネトロンスパッタリング装置。2. The target is formed in a substantially circular shape, and a rotary stage is provided so as to be rotatable along the back surface of the target, and is eccentric from the center of rotation of the rotary stage to 1/2 or more of the diameter of the target. A plurality of permanent magnets arranged in concentric circles having a diameter of 10 mm, and the plurality of permanent magnets can be moved toward and away from the back surface of the target on the side facing the vicinity of the center of the back surface. The magnetron sputtering apparatus according to claim 1, wherein the magnetron sputtering apparatus is attached to the rotary stage.
ーゲットの背後にこれに沿って回転する複数個の永久磁
石を設けて該ターゲットの前方に閉ループの磁界を形成
するマグネトロンスパッタリング装置に於いて、該複数
個の永久磁石とターゲットとの間に部分的に磁性体を介
在させて該ターゲットの表面の磁界強度を部分的に弱め
たことを特徴とするマグネトロンスパッタリング装置。3. A magnetron sputtering apparatus in which a target is provided facing a substrate, and a plurality of permanent magnets rotating along the target are provided behind the target to form a closed loop magnetic field in front of the target. A magnetron sputtering apparatus characterized in that a magnetic material is partially interposed between the plurality of permanent magnets and the target to partially weaken the magnetic field strength on the surface of the target.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP31213393A JPH07166346A (en) | 1993-12-13 | 1993-12-13 | Magnetron sputtering device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP31213393A JPH07166346A (en) | 1993-12-13 | 1993-12-13 | Magnetron sputtering device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH07166346A true JPH07166346A (en) | 1995-06-27 |
Family
ID=18025655
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP31213393A Pending JPH07166346A (en) | 1993-12-13 | 1993-12-13 | Magnetron sputtering device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH07166346A (en) |
Cited By (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR970067607A (en) * | 1996-03-13 | 1997-10-13 | 조셉 제이. 스위니 | Magnetron for Low Pressure Full Surface Corrosion |
US5919345A (en) * | 1994-09-27 | 1999-07-06 | Applied Materials, Inc. | Uniform film thickness deposition of sputtered materials |
US6042706A (en) * | 1997-01-14 | 2000-03-28 | Applied Materials, Inc. | Ionized PVD source to produce uniform low-particle deposition |
EP0820088A3 (en) * | 1996-07-19 | 2000-10-25 | Applied Komatsu Technology, Inc. | Non-planar magnet tracking device for magnetron sputtering apparatus |
US6183614B1 (en) | 1999-02-12 | 2001-02-06 | Applied Materials, Inc. | Rotating sputter magnetron assembly |
US6290825B1 (en) | 1999-02-12 | 2001-09-18 | Applied Materials, Inc. | High-density plasma source for ionized metal deposition |
US6497802B2 (en) | 1999-02-12 | 2002-12-24 | Applied Materials, Inc. | Self ionized plasma sputtering |
GB2379670A (en) * | 2001-09-12 | 2003-03-19 | Samsung Electronics Co Ltd | Sputtering Apparatus Using a Magnetic Field |
US6790323B2 (en) | 1999-02-12 | 2004-09-14 | Applied Materials, Inc. | Self ionized sputtering using a high density plasma source |
JP2004269952A (en) * | 2003-03-07 | 2004-09-30 | Showa Shinku:Kk | Magnetron sputtering mechanism and method therefor |
US7115194B2 (en) * | 2002-09-30 | 2006-10-03 | Victor Company Of Japan, Ltd. | Magnetron sputtering apparatus |
JP2007284794A (en) * | 2006-04-19 | 2007-11-01 | Maxim Integrated Products Inc | Plasma systems with magnetic filter devices to alter film deposition/etching characteristics |
JP2012201910A (en) * | 2011-03-24 | 2012-10-22 | Ulvac Japan Ltd | Magnetron sputtering electrode and sputtering apparatus |
US8778144B2 (en) * | 2004-09-28 | 2014-07-15 | Oerlikon Advanced Technologies Ag | Method for manufacturing magnetron coated substrates and magnetron sputter source |
KR102105868B1 (en) | 2018-10-24 | 2020-04-29 | 가부시키가이샤 알박 | Cathode device and sputtering device |
WO2020097815A1 (en) | 2018-11-14 | 2020-05-22 | Applied Materials, Inc. | Tilted magnetron in a pvd sputtering deposition chamber |
-
1993
- 1993-12-13 JP JP31213393A patent/JPH07166346A/en active Pending
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Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5919345A (en) * | 1994-09-27 | 1999-07-06 | Applied Materials, Inc. | Uniform film thickness deposition of sputtered materials |
US6228235B1 (en) | 1996-03-13 | 2001-05-08 | Applied Materials, Inc. | Magnetron for low pressure, full face erosion |
US5907220A (en) * | 1996-03-13 | 1999-05-25 | Applied Materials, Inc. | Magnetron for low pressure full face erosion |
KR970067607A (en) * | 1996-03-13 | 1997-10-13 | 조셉 제이. 스위니 | Magnetron for Low Pressure Full Surface Corrosion |
EP0820088A3 (en) * | 1996-07-19 | 2000-10-25 | Applied Komatsu Technology, Inc. | Non-planar magnet tracking device for magnetron sputtering apparatus |
US6042706A (en) * | 1997-01-14 | 2000-03-28 | Applied Materials, Inc. | Ionized PVD source to produce uniform low-particle deposition |
US6790323B2 (en) | 1999-02-12 | 2004-09-14 | Applied Materials, Inc. | Self ionized sputtering using a high density plasma source |
US6497802B2 (en) | 1999-02-12 | 2002-12-24 | Applied Materials, Inc. | Self ionized plasma sputtering |
US6183614B1 (en) | 1999-02-12 | 2001-02-06 | Applied Materials, Inc. | Rotating sputter magnetron assembly |
US6290825B1 (en) | 1999-02-12 | 2001-09-18 | Applied Materials, Inc. | High-density plasma source for ionized metal deposition |
GB2379670A (en) * | 2001-09-12 | 2003-03-19 | Samsung Electronics Co Ltd | Sputtering Apparatus Using a Magnetic Field |
GB2379670B (en) * | 2001-09-12 | 2003-10-22 | Samsung Electronics Co Ltd | Sputtering apparatus for forming a metal film using a magnetic field |
US6723215B2 (en) | 2001-09-12 | 2004-04-20 | Samsung Electronics Co., Ltd. | Sputtering apparatus for forming a metal film using a magnetic field |
DE10215369B4 (en) * | 2001-09-12 | 2009-03-26 | Samsung Electronics Co., Ltd., Suwon | Sputtering apparatus for forming a metal film using a magnetic field |
US7115194B2 (en) * | 2002-09-30 | 2006-10-03 | Victor Company Of Japan, Ltd. | Magnetron sputtering apparatus |
JP2004269952A (en) * | 2003-03-07 | 2004-09-30 | Showa Shinku:Kk | Magnetron sputtering mechanism and method therefor |
US8778144B2 (en) * | 2004-09-28 | 2014-07-15 | Oerlikon Advanced Technologies Ag | Method for manufacturing magnetron coated substrates and magnetron sputter source |
JP2007284794A (en) * | 2006-04-19 | 2007-11-01 | Maxim Integrated Products Inc | Plasma systems with magnetic filter devices to alter film deposition/etching characteristics |
JP2012201910A (en) * | 2011-03-24 | 2012-10-22 | Ulvac Japan Ltd | Magnetron sputtering electrode and sputtering apparatus |
KR102105868B1 (en) | 2018-10-24 | 2020-04-29 | 가부시키가이샤 알박 | Cathode device and sputtering device |
US10934616B2 (en) | 2018-10-24 | 2021-03-02 | Ulvac, Inc. | Cathode device and sputtering apparatus |
WO2020097815A1 (en) | 2018-11-14 | 2020-05-22 | Applied Materials, Inc. | Tilted magnetron in a pvd sputtering deposition chamber |
EP3880862A4 (en) * | 2018-11-14 | 2022-06-01 | Applied Materials, Inc. | Tilted magnetron in a pvd sputtering deposition chamber |
US11784032B2 (en) | 2018-11-14 | 2023-10-10 | Applied Materials, Inc. | Tilted magnetron in a PVD sputtering deposition chamber |
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