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JPH0362789B2 - - Google Patents
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JPH0362789B2 - - Google Patents

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Publication number
JPH0362789B2
JPH0362789B2 JP30614387A JP30614387A JPH0362789B2 JP H0362789 B2 JPH0362789 B2 JP H0362789B2 JP 30614387 A JP30614387 A JP 30614387A JP 30614387 A JP30614387 A JP 30614387A JP H0362789 B2 JPH0362789 B2 JP H0362789B2
Authority
JP
Japan
Prior art keywords
magnetic
target
plate
magnetron sputtering
present
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.)
Expired
Application number
JP30614387A
Other languages
Japanese (ja)
Other versions
JPH01147063A (en
Inventor
Kyuzo Nakamura
Yoshifumi Oota
Yasushi Higuchi
Akira Ishibashi
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.)
Ulvac Inc
Original Assignee
Ulvac Inc
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 Ulvac Inc filed Critical Ulvac Inc
Priority to JP30614387A priority Critical patent/JPH01147063A/en
Publication of JPH01147063A publication Critical patent/JPH01147063A/en
Publication of JPH0362789B2 publication Critical patent/JPH0362789B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は基板に薄膜を形成するのに用いられる
マグネトロン・スパツタ装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to magnetron sputtering equipment used to form thin films on substrates.

〔従来の技術及びその問題点〕[Conventional technology and its problems]

マグネトロン・スパツタ装置は、基板にターゲ
ツトの材料を効率よく、その薄膜を形成させるの
に用いられるものであるが、第7図はこの一従来
例を示し、磁性材で成るヨーク1上に磁極2a,
2b及び中心磁極3が形成されている。本例で
は、これらは永久磁石から成るもので、断面は山
形を呈しているが、実際には中心磁極3を同心的
に外側磁極2a,2bが形成されている。すなわ
ち2aと2bは一体的となつている。中心磁極3
は上方がN極、下方がS極であり、この外方の2
a,2bは上方がS極、下方がN極となつてい
る。従つて、中心の磁極3から矢印Hで示すよう
に、磁力線Hが外側磁極2a,2bに流入するよ
うになつている。なお本例では、永久磁石で磁界
発生装置を構成する場合を説明したが、これは電
磁石で構成しててもよい。この場合には中心磁極
N−Sの周囲にコイルが巻装されることになる。
磁極2a,2b,3に近接して、ターゲツト支持
板4が配設され、これにターゲツト5が支持され
ている。磁力線Hは磁極2aと3、又は3と2a
との間で、その方向がターゲツト5の面に対し
ほゞ平行になるために、この部分において、プラ
ズマが集中するようになつている。従つて、この
ターゲツトからイオンが飛び出すのは、ハツチン
グで示した部分5a,5bが圭とした部分であ
り、従つてこゝが支配的に侵食される(エロージ
ヨン)。そして、そと他の部分においては、ハツ
チングで示されてないように、ほとんど侵食され
ることはなく、このターゲツトを有効に利用して
いるとは言えない。すなわちその利用効率は非常
に低いものである。
A magnetron sputtering device is used to efficiently form a thin film of target material on a substrate. FIG. 7 shows a conventional example of this, in which a magnetic pole 2a is placed on a yoke 1 made of a magnetic material. ,
2b and a central magnetic pole 3 are formed. In this example, these are made of permanent magnets and have a chevron-shaped cross section, but in reality, outer magnetic poles 2a and 2b are formed concentrically with the center magnetic pole 3. In other words, 2a and 2b are integrated. Center magnetic pole 3
The upper part is the north pole and the lower part is the south pole, and these two outer
The upper part of a and 2b is the south pole, and the lower part is the north pole. Therefore, lines of magnetic force H flow from the central magnetic pole 3 to the outer magnetic poles 2a, 2b as shown by arrows H. In this example, a case has been described in which the magnetic field generator is configured with permanent magnets, but it may also be configured with electromagnets. In this case, a coil is wound around the central magnetic pole N-S.
A target support plate 4 is disposed adjacent to the magnetic poles 2a, 2b, and 3, and a target 5 is supported on this. The lines of magnetic force H are magnetic poles 2a and 3, or 3 and 2a
Since the direction between the two points is approximately parallel to the surface of the target 5, the plasma is concentrated in this area. Therefore, the ions eject from this target at the hatched portions 5a and 5b, and therefore the levers are dominantly eroded (erosion). In other parts, as shown by the hatching, there is almost no erosion, and it cannot be said that this target is used effectively. In other words, its utilization efficiency is extremely low.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

本発明は以上の問題に鑑みてなされ、ターゲツ
トの使用効率の大きいマグネトロン・スパツタ装
置を提供することを目的とする。
The present invention has been made in view of the above problems, and an object of the present invention is to provide a magnetron sputtering device with high target usage efficiency.

〔作用〕[Effect]

複数の空〓又は磁気抵抗の特に大きい部分に対
抗する位置で平行磁界の強度が最大となる。この
ような空〓又は磁気抵抗の特に大きい部分が複
数、設けられることにより平行磁界の強い部分が
広がり、よつてターゲツトのエロージヨンは従来
より一段と均一化される。すなわち、ターゲツト
の利用効率を向上させることができる。
The strength of the parallel magnetic field is maximum at a position opposing a plurality of spaces or a particularly large portion of magnetic resistance. By providing a plurality of such regions or regions with particularly high magnetic resistance, the region with a strong parallel magnetic field is spread out, and the erosion of the target is thus made more uniform than in the past. In other words, it is possible to improve the target usage efficiency.

〔実施例〕〔Example〕

以下、本発明の実施例によるマグネトロン・ス
パツタ装置について、第1図乃至第6図を参照し
て説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS A magnetron sputtering apparatus according to an embodiment of the present invention will be described below with reference to FIGS. 1 to 6.

第1図乃至第3図は本発明の第1実施例を示す
ものであるが、第7図の従来例に対応する部分に
ついては同一の符号を付し、その詳細にな説明は
省略する。
1 to 3 show a first embodiment of the present invention, parts corresponding to the conventional example in FIG. 7 are designated by the same reference numerals, and detailed explanation thereof will be omitted.

すなわち本実施例の磁界発生装置は永久磁石で
構成され、その形状は同心円状である。そして、
この永久磁石の磁極2a,2b,3にわずかな空
〓をおいて、ターゲツト支持板10(いわゆるバ
ツキングプレート)が配設される。これは従来例
と同様に、磁性材ではない他の金属であり例え
ば、銅で成るものである。そしてこの上にターゲ
ツト5が支持される。そして本発明によれば、タ
ーゲツト支持板10に第2図に示すような形状の
磁性板11が埋設されている。すなわち、本実施
例の磁性板11は、同心状態に形成され、中心部
11a、これと同心的な中間部11b及びこれと
同心的な外周部11cから成つており、これらの
間に間〓12a,12bを形成させている。本発
明の第1実施例は以上のように構成されるのであ
るが、次にこの作用について説明する。永久磁石
の磁極3からは、第1図の矢印で示すように、磁
力線H′が流出し、大部分は中間磁性板部11b
へと流入し、これから外方の磁極部2a,2bへ
と外周部11cを介して流入する。そして部分的
に磁極3から外方の磁極2a,2bへ流れる。す
なわち、従来は殆んど全ての磁力線が中央の電極
3から、直接、外方の磁極2a,2bへ流れてい
つたのであるが、本実施例によれば、図で示すよ
うな磁力線のいわゆる短絡路が形成される。従つ
てこのような磁力線について、その垂直成分と平
行成分についてグラフで示せば、第3図のように
なる。この図から明らかなように垂直成分は、タ
ーゲツト5の両端部において最大値を示し、これ
から内方に向うにつれて急激に減少し、空〓12
a,12bに対応する部分でほとんどゼロとな
り、そしてターゲツト5の中心部では極大値を示
している。また、磁力線の平行成分については、
ターゲツト5の中心とターゲツト5端部の間で、
ほゞ一様なレベルを示している。これを第4図に
示す従来の各成分と比較してみると、従来では平
行成分はターゲツトの中心部とターゲツトの端部
とのほゞ中間部において局在していたが、これが
本実施例によれば、第3図に示すごとく、ほゞ一
様に分布されている。また従来例では垂直成分や
はりターゲツトの中心、乃びターゲツト端部にお
いて極大値を示しているが、ターゲツト中心とタ
ーゲツト端部の中心部分でほゞゼロとなつてい
る。
That is, the magnetic field generating device of this embodiment is composed of a permanent magnet, and its shape is concentric circles. and,
A target support plate 10 (so-called bucking plate) is provided with a slight gap between the magnetic poles 2a, 2b, and 3 of the permanent magnets. Similar to the conventional example, this material is made of a metal other than a magnetic material, such as copper. The target 5 is then supported on top of this. According to the present invention, a magnetic plate 11 having a shape as shown in FIG. 2 is embedded in the target support plate 10. That is, the magnetic plate 11 of this embodiment is formed concentrically and consists of a center portion 11a, an intermediate portion 11b concentric with the center portion, and an outer peripheral portion 11c concentric with the center portion 11a, with a gap 12a between them. , 12b are formed. The first embodiment of the present invention is constructed as described above, and its operation will be explained next. From the magnetic pole 3 of the permanent magnet, lines of magnetic force H' flow out, as shown by the arrows in FIG.
From there, it flows into the outer magnetic pole parts 2a and 2b via the outer peripheral part 11c. Then, it partially flows from the magnetic pole 3 to the outer magnetic poles 2a and 2b. That is, in the past, almost all the lines of magnetic force flowed directly from the central electrode 3 to the outer magnetic poles 2a and 2b, but according to this embodiment, the so-called short circuit of the lines of magnetic force as shown in the figure A path is formed. Therefore, if the perpendicular and parallel components of such lines of magnetic force are shown graphically, the result will be as shown in FIG. As is clear from this figure, the vertical component shows a maximum value at both ends of the target 5, and then rapidly decreases as it moves inward, until the vertical component reaches its maximum value at both ends of the target 5.
It becomes almost zero in the parts corresponding to a and 12b, and shows a maximum value in the center of target 5. Also, regarding the parallel components of magnetic field lines,
Between the center of target 5 and the end of target 5,
It shows almost uniform level. Comparing this with the conventional components shown in FIG. 4, it is found that in the conventional method, the parallel component was localized approximately in the middle between the center of the target and the end of the target, but this is different from that in this embodiment. According to the method, as shown in FIG. 3, the distribution is almost uniform. Further, in the conventional example, the vertical component also shows a maximum value at the center of the target and at the end of the target, but it becomes almost zero at the center of the target and the center of the end of the target.

本実施例によれば以上のような磁界分布を示す
ので、第1図に示すようなエロージヨン13a,
13bが形成され、ターゲツト5は一様に侵食さ
れることになることにより、その用効率は従来と
比べるとはるかに高いものである。
According to this embodiment, since the magnetic field distribution as described above is shown, the erosion 13a, as shown in FIG.
13b is formed and the target 5 is uniformly eroded, so that its usage efficiency is much higher than in the past.

以上の実施例で、例えば磁性板11の厚みを3
m/mとし、これをパーマロイで形成し、間〓1
2a,12b幅を10m/mとし、またターゲツト
5の径を6インチφ、その厚みを6mmでクロム
(Cr)で成るものとすれば、ターゲツト5の使用
高率は55%であつたが、同じ材料、かつ同じサイ
ズで従来例ではその使用効率は25%であつた。
In the above embodiment, for example, the thickness of the magnetic plate 11 is set to 3
m/m, this is made of permalloy, and the distance is 1
If the width of targets 2a and 12b is 10 m/m, and the diameter of target 5 is 6 inches, the thickness is 6 mm, and it is made of chromium (Cr), the usage rate of target 5 is 55%. In the conventional example using the same material and size, the usage efficiency was 25%.

第5図は本発明の第2実施例によるマグネトロ
ン・スパツタ装置における、要部である磁性板2
0の平面形状を示すものである。すなわち本実施
例では、上述の実施例の永久磁石が同心円状であ
つたのに対し、ターゲツトが長方形状であり、こ
れに対応して永久磁石も長方形状となつており、
その中心部に第5図に示すように磁性板20の中
心部23に対向する位置に中心磁極があり、これ
と長方形状であるが同心的に外周の磁極が磁性板
20の外周部21に対向して構成されている。そ
してこの磁性板20は、すでに述べたように中心
部23、中間部22、及び外周部21から成つて
おり、これらの間には空〓24,25が形成され
ている。このような実施例でも第1実施例と同様
な効果を得ることは明らかである。
FIG. 5 shows a magnetic plate 2 which is a main part in a magnetron sputtering device according to a second embodiment of the present invention.
This shows the planar shape of 0. That is, in this example, whereas the permanent magnets of the above-mentioned examples were concentric, the target was rectangular, and the permanent magnet was also rectangular correspondingly.
As shown in FIG. 5, there is a central magnetic pole in the center facing the central part 23 of the magnetic plate 20, and a rectangular outer magnetic pole is located concentrically with the outer peripheral part 21 of the magnetic plate 20. They are configured to face each other. As described above, this magnetic plate 20 is composed of a central portion 23, an intermediate portion 22, and an outer circumferential portion 21, and voids 24 and 25 are formed between these portions. It is clear that the same effects as in the first embodiment can be obtained in this embodiment as well.

第6図は本発明の第3実施例を示すものである
が、第1実施例に対応する部分については同一の
符号を付し、その詳細な説明は省略する。
FIG. 6 shows a third embodiment of the present invention, and parts corresponding to the first embodiment are denoted by the same reference numerals, and detailed explanation thereof will be omitted.

本実施例によれば、ターゲツト支持板30には
第1実施例と同様に磁性板31が埋設されてお
り、またこれは第1実施例と同様に同心的な形状
を有するものであるが、その中心部32と外周部
33との厚みは、中間部34の厚みより大きくし
てその磁気抵抗をより小なるものとしている。こ
のようにすれば、磁極3から2a,2bに向う磁
気抵抗がより小さくなつて磁束をより強くするこ
とができ、かつ上記実施例で述べた効果を奏する
ものである。
According to this embodiment, a magnetic plate 31 is embedded in the target support plate 30 as in the first embodiment, and this has a concentric shape as in the first embodiment. The thickness of the center portion 32 and the outer peripheral portion 33 is made larger than the thickness of the intermediate portion 34 to further reduce the magnetic resistance. In this way, the magnetic resistance from the magnetic poles 3 toward 2a and 2b becomes smaller, the magnetic flux can be made stronger, and the effects described in the above embodiments can be achieved.

以上本発明の各実施例について説明したが、も
ちろん本発明はこれらに限定されることなく、本
発明の技術的思想に基づいて種々の変形が可能で
ある。
Although each embodiment of the present invention has been described above, the present invention is of course not limited to these, and various modifications can be made based on the technical idea of the present invention.

例えば、以上の実施例では磁性板11,20,
30には2つの空〓が形成されたがさらにこれを
増加するようにしてもよい。すなわち、以上の実
施例では磁性板は、分割構造としたが、この分割
数をさらに増大させるようにしてもよい。
For example, in the above embodiment, the magnetic plates 11, 20,
Although two vacancies are formed at 30, the number may be further increased. That is, in the above embodiment, the magnetic plate has a divided structure, but the number of divisions may be further increased.

また、以上の実施例では、磁性板に複数の空〓
を形成させるようにしたが、これに代えてこの部
分をごく薄くするようにしてもよい。すなわち、
この部分を特に大きい磁気抵抗を有するようにし
ても空〓の場合より効果は小さくなるが、従来よ
りは利用効率を高めることができる。あるいはこ
れに代えて、空〓部分の非磁性材で成る材料で充
てんさせたものであつてもよい。すなわち、例え
ば同心状に成る分割磁性材の各空〓部分に非磁性
材で成る、同じく同心的な材料で充充填させるよ
うにして完全に一体物とし、これをターゲツト支
持板を表面に貼着させるようにしてもよい。ある
いはこのような磁性材、あるいは実施例で示すよ
うな形状の磁性板を磁界発生装置とターゲツト支
持板の間に介設させるようにしてもよい。
In addition, in the above embodiment, a plurality of air holes are provided on the magnetic plate.
However, instead of this, this portion may be made very thin. That is,
Even if this part is made to have a particularly large magnetic resistance, the effect will be smaller than in the case of an empty space, but the utilization efficiency can be improved compared to the conventional case. Alternatively, the empty portion may be filled with a material made of a non-magnetic material. That is, for example, each hollow part of a concentric divided magnetic material is filled with a concentric material made of a non-magnetic material to form a completely integrated object, and a target support plate is attached to the surface. You may also do so. Alternatively, such a magnetic material or a magnetic plate having a shape as shown in the embodiment may be interposed between the magnetic field generator and the target support plate.

また、以上の実施例では磁性板の材料としてパ
ーマロイが用いられたが、他の磁性材であつても
よいが透磁率の高い材質で好ましい。
Further, in the above embodiments, permalloy was used as the material of the magnetic plate, but other magnetic materials may be used, but materials with high magnetic permeability are preferred.

また、以上の実施例では磁界発生装置としては
永久磁石を用いたが、冒頭で述べたように電磁石
であつてもよい。またその磁石の形状も同心円的
なものではなく、断面形状が同じくE型であつて
も中心磁極の両側に対向する磁極が相独立した磁
極であつても同様な効果が得られることはもちろ
んである。
Further, in the above embodiments, a permanent magnet is used as the magnetic field generating device, but as mentioned at the beginning, an electromagnet may be used. Moreover, the shape of the magnet is not concentric, and even if the cross-sectional shape is E-shaped, the same effect can be obtained even if the magnetic poles facing on both sides of the central magnetic pole are independent magnetic poles. be.

〔発明の効果〕〔Effect of the invention〕

以上述べたように本発明のマグネトロン・スパ
ツタ装置によれば、従来に比べターゲツトの利用
効率を一段と向上させることができ、よつて生産
コストを低下させることができる。また、ターゲ
ツトの交換のインターバルを従来より長くするこ
とができる。
As described above, according to the magnetron sputtering apparatus of the present invention, it is possible to further improve the efficiency of target utilization compared to the conventional method, thereby reducing production costs. Furthermore, the interval between target exchanges can be made longer than before.

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

第1図は本発明の第1実施例によるマグトロ
ン・スパツタ装置の部分断面側面図、第2図は第
1図における磁性板の平面図、第3図は同実施例
の作用を説明するためのグラフ、第4図は同実施
例の作用と比較するための従来例の作用を示すグ
ラフ、第5図は本発明の第2実施例のマグネトロ
ン・スパツタ装置に用いられる磁性板の平面図、
第6図は本発明の第3実施例によるマグネトロ
ン・スパツタ装置の部分断面側面図、及び第7図
は従来例のマグネトロン・スパツタ装置の部分断
面側面図である。 なお図において、11,20,31……磁性
材。
FIG. 1 is a partially sectional side view of a magtron sputtering device according to a first embodiment of the present invention, FIG. 2 is a plan view of the magnetic plate in FIG. 1, and FIG. 3 is a diagram for explaining the operation of the same embodiment. Graph, FIG. 4 is a graph showing the effect of the conventional example for comparison with the effect of the same embodiment, FIG. 5 is a plan view of the magnetic plate used in the magnetron sputtering device of the second embodiment of the present invention,
FIG. 6 is a partially sectional side view of a magnetron sputtering device according to a third embodiment of the present invention, and FIG. 7 is a partially sectional side view of a conventional magnetron sputtering device. In the figure, 11, 20, 31...magnetic materials.

Claims (1)

【特許請求の範囲】 1 磁界発生装置とこれに近接してターゲツトと
を備えたマグネトロン・スパツタ装置において、
前記磁界発生装置と前記ターゲツトとの間に板状
の磁性部材を介設し、その前記磁界発生装置の磁
極間に対向する部位に複数の空〓又は磁気抵抗の
特に大きい部分を形成させるようにしたことを特
徴とするマグネトロン・スパツタ装置。 2 前記ターゲツトの支持板に前記磁性部材を取
付けた前記第1項に記載のマグネトロン・スパツ
タ装置。
[Claims] 1. A magnetron sputtering device comprising a magnetic field generating device and a target adjacent thereto,
A plate-shaped magnetic member is interposed between the magnetic field generating device and the target, and a plurality of voids or parts with particularly high magnetic resistance are formed at a portion facing between the magnetic poles of the magnetic field generating device. A magnetron spatuta device that is characterized by: 2. The magnetron sputtering device according to item 1 above, wherein the magnetic member is attached to the support plate of the target.
JP30614387A 1987-12-03 1987-12-03 Magnetron sputtering device Granted JPH01147063A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30614387A JPH01147063A (en) 1987-12-03 1987-12-03 Magnetron sputtering device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30614387A JPH01147063A (en) 1987-12-03 1987-12-03 Magnetron sputtering device

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JPH01147063A JPH01147063A (en) 1989-06-08
JPH0362789B2 true JPH0362789B2 (en) 1991-09-27

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JP30614387A Granted JPH01147063A (en) 1987-12-03 1987-12-03 Magnetron sputtering device

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Publication number Priority date Publication date Assignee Title
DE19622607B4 (en) * 1996-06-05 2007-12-27 Oerlikon Deutschland Holding Gmbh sputter cathode
DE19622606C2 (en) * 1996-06-05 2002-02-28 Applied Films Gmbh & Co Kg sputter cathode
DE19747923C2 (en) * 1997-10-30 2002-09-12 Leybold Systems Gmbh sputter cathode
DE19754986C2 (en) * 1997-12-11 2002-09-12 Leybold Systems Gmbh sputter cathode
US7485210B2 (en) * 2004-10-07 2009-02-03 International Business Machines Corporation Sputtering target fixture
EP2067874B1 (en) 2007-11-29 2011-03-02 W.C. Heraeus GmbH Magnetic shunts in tube targets
DE102007060306B4 (en) 2007-11-29 2011-12-15 W.C. Heraeus Gmbh Magnetic shunts in tube targets
US20110108416A1 (en) * 2009-11-10 2011-05-12 Cheng-Tsung Liu Magnetron sputter
WO2012102092A1 (en) * 2011-01-24 2012-08-02 日立金属株式会社 Magnetic field generation device for magnetron sputtering
DE112012001988T5 (en) 2011-05-30 2014-02-20 Hitachi Metals Ltd. Racetrack-shaped magnetic field generating device for magnetron sputtering
WO2013115030A1 (en) 2012-01-30 2013-08-08 日立金属株式会社 Magnetic field generator for magnetron sputtering
TW201335405A (en) * 2012-02-24 2013-09-01 Sumika Technology Co Ltd Composite target and method of manufacturing the same
WO2015090373A1 (en) * 2013-12-17 2015-06-25 Applied Materials, Inc. Electrode assembly for deposition apparatus and method for assembling said electrode assembly

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