JPS63282263A - Magnetron sputtering device - Google Patents
Magnetron sputtering deviceInfo
- Publication number
- JPS63282263A JPS63282263A JP11660387A JP11660387A JPS63282263A JP S63282263 A JPS63282263 A JP S63282263A JP 11660387 A JP11660387 A JP 11660387A JP 11660387 A JP11660387 A JP 11660387A JP S63282263 A JPS63282263 A JP S63282263A
- Authority
- JP
- Japan
- Prior art keywords
- target
- magnet
- center
- pole
- 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.)
- Pending
Links
- 238000001755 magnetron sputter deposition Methods 0.000 title claims description 7
- 230000003628 erosive effect Effects 0.000 abstract description 4
- 230000002708 enhancing effect Effects 0.000 abstract 1
- 239000000758 substrate Substances 0.000 description 8
- 239000002245 particle Substances 0.000 description 4
- 238000004544 sputter deposition Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、電界とそれに直交する磁界により高密度のプ
ラズマを発生させ、ターゲットを叩いて高い被着速度を
得るマグネトロンスパッタリング装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a magnetron sputtering apparatus that generates high-density plasma using an electric field and a magnetic field perpendicular to the electric field and strikes a target to obtain a high deposition rate.
従来のマグネトロン装置は、第2図に示すように真空容
器1の中に直流電源2に接続された陰極3と接地された
陽極4が対向配置され、陰極3には被着材料からなるタ
ーゲット5.陽極4には成膜基板6が取り付けられる。In a conventional magnetron device, as shown in FIG. 2, a cathode 3 connected to a DC power source 2 and a grounded anode 4 are disposed facing each other in a vacuum vessel 1, and a target 5 made of an adhering material is attached to the cathode 3. .. A film-forming substrate 6 is attached to the anode 4 .
この装置の真空容器1を排気ロアより排気し、ガス導入
口8からArガスを導入し、さらに両極3.4間に電圧
を印加して放電を起こす、放電によって電離した電子を
ターゲットから出てターゲットに入る磁界によって閉じ
こめ、高密度のプラズマを発生させ、Ar” 9をター
ゲット5に衝突させて、ターゲットから叩き出された粒
子を基板6上に堆積させる。The vacuum chamber 1 of this device is evacuated from the exhaust lower, Ar gas is introduced from the gas inlet 8, and a voltage is applied between the two electrodes 3.4 to cause a discharge.The electrons ionized by the discharge are ejected from the target. It is confined by a magnetic field entering the target to generate a high-density plasma, and Ar'' 9 is made to collide with the target 5, causing particles ejected from the target to be deposited on the substrate 6.
ターゲットから出てターゲットへ入る磁界を形成するに
は、陰極の背面に配置されたマグネットが用いられる。A magnet placed behind the cathode is used to create a magnetic field that exits and enters the target.
そのマグネットは、一方の極が中央で他方の極はそれを
囲む円環状であるため、プラズマは両極の間の上の環状
領域に発生し、従って第3図に示すようにターゲット5
のエロージッン領域51は環状であり、中央部が残るた
め、ターゲットの利用効率は30〜50%程度に留まり
、夕一ゲントの交換による頻繁なメンテナンスがスパッ
タリング装置の稼働率を低下させる点で大きな問題とな
っている。また、このように基板6に対向するターゲッ
ト5のエロージッン領域が一部分に限定されるため、タ
ーゲットから飛来する粒子が基板に垂直に当たることが
少な(なる、最近半導体素子の微細化により、第4図に
示すように半導体基板上の絶縁膜41に形成されるコン
タクトホール42のアスペクト比T r / T zが
1以上になって(ると、スパッタ粒子の入射方向43の
基板面に立てた垂線44となす入射角θがOであること
がコンタクトホール42の底部被覆のために望ましく、
この面でも問題となっている。Since the magnet has an annular shape with one pole in the center and the other pole surrounding it, the plasma is generated in the upper annular region between the two poles, so that the target 5 as shown in FIG.
The erosion region 51 is annular and the central part remains, so the target utilization efficiency remains at about 30 to 50%, which is a big problem in that frequent maintenance due to replacement of the sputtering device reduces the operating rate of the sputtering equipment. It becomes. In addition, since the erosion region of the target 5 facing the substrate 6 is limited to a portion, particles flying from the target rarely hit the substrate perpendicularly (recently, due to the miniaturization of semiconductor devices, As shown in , when the aspect ratio T r /T z of the contact hole 42 formed in the insulating film 41 on the semiconductor substrate becomes 1 or more (then, the perpendicular line 44 erected on the substrate surface in the incident direction 43 of the sputtered particles It is desirable that the incident angle θ is O in order to cover the bottom of the contact hole 42.
This is also a problem.
本発明の目的は、上記の問題を解決し、スパッタターゲ
ットのエロージョン領域を拡大してターゲット利用効率
を上げ、ターゲット交換による利用効率の低下を防ぎ、
かつ高アスペクト比の素子においてコンタクトホール部
の底部の被覆性を向上させることのできるマグネトロン
スパッタリング装置を提供することにある。The purpose of the present invention is to solve the above problems, increase the target utilization efficiency by expanding the erosion area of the sputter target, and prevent the decrease in utilization efficiency due to target replacement.
Another object of the present invention is to provide a magnetron sputtering device that can improve the coverage of the bottom of a contact hole in a high aspect ratio device.
上記の目的を達成するために、本発明は、真空容器内に
陽極に対向して配置される陰極の陽極側にターゲットが
取り付けられ、陰極の反ターゲット側に環状のマグネッ
トを備え、そのマグネットの一方の極がターゲットの中
心と外周の中間の背面に位置し、その極を取囲む他方の
極は少なくともターゲットの中心6冑面まで延びており
、かつマグネットがターゲットの中心軸線の周りに回動
可能であるものとする。In order to achieve the above object, the present invention includes a target attached to the anode side of a cathode placed opposite to the anode in a vacuum container, and an annular magnet provided on the opposite side of the cathode to the target. One pole is located on the back surface between the center and outer circumference of the target, and the other pole surrounding that pole extends at least to the center of the target, and the magnet rotates around the center axis of the target. It shall be possible.
環状のマグネットが陰極の反ターゲット側でターゲット
の中心軸線の周りに回動することにより、そのマグネッ
トによってターゲットから出てターゲットに入る磁力線
は、ターゲットの中心の周りのマグネットの外側の端部
の裏側に至る領域全体を覆い、その範囲のターゲツト面
がスパッタされる。従って、ターゲットの利用効率が高
くなる。By rotating the annular magnet around the center axis of the target on the anti-target side of the cathode, the magnetic field lines exiting and entering the target through that magnet are directed behind the outer end of the magnet around the center of the target. The target surface in that range is sputtered. Therefore, the target utilization efficiency becomes high.
第1図は本発明の一実施例において陰極の背面に取り付
けられるマグネットをターゲット側から見た透視平面図
で、周りに同一寸法のターゲット5および陰8i3の輪
郭を示す、マグネット10は環状で、中央にN極11.
外周に38i12が陰極面に垂直にターゲットに向けて
突出している。このマグネットにより、ターゲット5の
面上の点線の斜線で示した領域13に放射状に磁力線が
生ずる。ターゲット表面のこの領域に電子が閉じ込めら
れてターゲットのスパッタが行われる。従って、マグネ
ット10をターゲット5の中心軸50の周りに矢印14
のように回動させた場合、スパッタはターゲットの中心
を含むほぼ全面で行われ、第5図に示すようなエロージ
ッン領域51が生じ、ターゲット5の利用効率は70%
程度まで上がった。このマグネトロンスパッタリング装
置を用い、第6図に示す絶縁膜41の深さT I−1,
2Jlll1幅T* −1,Onのアスペクト比1.2
のコンタクトホール42にA143を堆積させたところ
、絶縁膜上面でのMの膜厚d、−0、5tnaに対しコ
ンタクトホール底部の膜厚d、−0,4−で膜厚比0.
8であり、また側面の膜厚ds=O,15jIsでカバ
レージ30%の数字が得られた。FIG. 1 is a perspective plan view of a magnet attached to the back surface of a cathode in an embodiment of the present invention, seen from the target side. The magnet 10 is annular and shows the outline of a target 5 and a shadow 8i3 having the same dimensions around it. N pole 11 in the center.
38i12 on the outer periphery protrudes toward the target perpendicularly to the cathode surface. Due to this magnet, lines of magnetic force are generated radially in a region 13 indicated by dotted diagonal lines on the surface of the target 5. Electrons are trapped in this region of the target surface and sputter the target. Therefore, the magnet 10 is moved around the central axis 50 of the target 5 by the arrow 14.
When the target is rotated as shown in FIG.
It has risen to a certain extent. Using this magnetron sputtering device, the depth T I-1 of the insulating film 41 shown in FIG.
2Jlll1 width T* -1, On aspect ratio 1.2
When A143 was deposited in the contact hole 42, the film thickness ratio of M at the top surface of the insulating film was d, -0, 5tna, whereas the film thickness at the bottom of the contact hole was d, -0, 4-, and the film thickness ratio was 0.
8, and a coverage of 30% was obtained with the side film thickness ds=O, 15jIs.
本発明によれば、マグネトロンスパッタリング装置のタ
ーゲットの背面に設置する環状マグネットを固定しない
で、その中央の極がターゲットの中心と外周部の中間の
背面でターゲットの中心軸の周りを回るように移動させ
ることにより、磁力&11w1域はターゲット表面でタ
ーゲット中心の周りの広い範囲に全面に生ずるため、タ
ーゲットの利用効率が上がってターゲット交換によるス
パッタリング装置稼働率の低下を防ぐと共に、ターゲッ
トから飛び出して成膜基板面に垂直に当たる粒子が増加
することにより、高アスペクト比のコンタクトホールの
底部の被覆性も向上させることができた。According to the present invention, the annular magnet installed on the back surface of the target of a magnetron sputtering device is not fixed, but moves so that its central pole revolves around the central axis of the target at the back surface midway between the center and outer circumference of the target. By doing so, the magnetic force &11w1 region is generated over a wide area around the target center on the target surface, which improves target usage efficiency and prevents decrease in sputtering equipment operating rate due to target replacement. By increasing the number of particles perpendicular to the substrate surface, it was also possible to improve the coverage of the bottoms of high aspect ratio contact holes.
第1図は本発明の一実施例におけるマグネット部の透視
平面図、第2図はマグネトロンスパッタリング装置の断
面図、第3図は従来の装置に用いたターゲットの断面図
、第4図はコンタクトホール部の断面図、第5図は本発
明の一実施例の装置に用いたターゲットの断面図、第6
図は本発明の一実施例の装置を用いてM膜を形成したコ
ンタクトホール部の断面図である。
1:真空容器、3:陰極、4:陽極、5:ターゲット、
6:成膜基板、10:マグネット、11:N極、12:
S極。
、+へ
第1図
第2図
第4図
第5図
■
第6図Fig. 1 is a perspective plan view of a magnet section in an embodiment of the present invention, Fig. 2 is a sectional view of a magnetron sputtering device, Fig. 3 is a sectional view of a target used in a conventional device, and Fig. 4 is a contact hole. FIG. 5 is a cross-sectional view of a target used in an apparatus according to an embodiment of the present invention, and FIG.
The figure is a cross-sectional view of a contact hole portion in which an M film is formed using an apparatus according to an embodiment of the present invention. 1: Vacuum vessel, 3: Cathode, 4: Anode, 5: Target,
6: Film forming substrate, 10: Magnet, 11: N pole, 12:
S pole. , to +Figure 1 Figure 2 Figure 4 Figure 5■ Figure 6
Claims (1)
側にターゲットが取り付けられ、陰極の反ターゲット側
に環状のマグネットを備え、該マグネットの一方の極が
ターゲットの中心と外周の中間の背面に位置し、該極を
取囲む他方の極が少なくともターゲットの中心の背面ま
で延びており、かつマグネットがターゲットの中心軸線
の周りに回動可能な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 target is attached to the anode side of a cathode placed opposite to the anode in a vacuum container, and a ring-shaped magnet is provided on the opposite side of the cathode to the target, with one pole of the magnet located midway between the center and the outer periphery of the target. A magnetron sputtering apparatus characterized in that the other pole surrounding the pole extends at least to the back surface of the center of the target, and the magnet is rotatable around the center axis of the target.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11660387A JPS63282263A (en) | 1987-05-13 | 1987-05-13 | Magnetron sputtering device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11660387A JPS63282263A (en) | 1987-05-13 | 1987-05-13 | Magnetron sputtering device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63282263A true JPS63282263A (en) | 1988-11-18 |
Family
ID=14691247
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11660387A Pending JPS63282263A (en) | 1987-05-13 | 1987-05-13 | Magnetron sputtering device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63282263A (en) |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5120417A (en) * | 1990-02-28 | 1992-06-09 | Anelva Corporation | Magnetron sputtering apparatus and thin film depositing method |
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 |
US6306265B1 (en) | 1999-02-12 | 2001-10-23 | Applied Materials, Inc. | High-density plasma for ionized metal deposition capable of exciting a plasma wave |
US6358376B1 (en) * | 2000-07-10 | 2002-03-19 | Applied Materials, Inc. | Biased shield in a magnetron sputter reactor |
US6440282B1 (en) | 1999-07-06 | 2002-08-27 | Applied Materials, Inc. | Sputtering reactor and method of using an unbalanced magnetron |
US6497802B2 (en) | 1999-02-12 | 2002-12-24 | Applied Materials, Inc. | Self ionized plasma sputtering |
US6663754B2 (en) | 2001-04-13 | 2003-12-16 | Applied Materials, Inc. | Tubular magnet as center pole in unbalanced sputtering magnetron |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6199673A (en) * | 1984-10-15 | 1986-05-17 | Tokuda Seisakusho Ltd | Sputtering device |
JPS62230970A (en) * | 1986-03-31 | 1987-10-09 | Shimadzu Corp | Device for sputtering magnetron |
-
1987
- 1987-05-13 JP JP11660387A patent/JPS63282263A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6199673A (en) * | 1984-10-15 | 1986-05-17 | Tokuda Seisakusho Ltd | Sputtering device |
JPS62230970A (en) * | 1986-03-31 | 1987-10-09 | Shimadzu Corp | Device for sputtering magnetron |
Cited By (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5120417A (en) * | 1990-02-28 | 1992-06-09 | Anelva Corporation | Magnetron sputtering apparatus and thin film depositing method |
US6790323B2 (en) | 1999-02-12 | 2004-09-14 | Applied Materials, Inc. | Self ionized sputtering using a high density plasma source |
US6183614B1 (en) * | 1999-02-12 | 2001-02-06 | Applied Materials, Inc. | Rotating sputter magnetron assembly |
JP4837832B2 (en) * | 1999-02-12 | 2011-12-14 | アプライド マテリアルズ インコーポレイテッド | High density plasma source for ionized metal deposition. |
US6290825B1 (en) * | 1999-02-12 | 2001-09-18 | Applied Materials, Inc. | High-density plasma source for ionized metal deposition |
US6306265B1 (en) | 1999-02-12 | 2001-10-23 | Applied Materials, Inc. | High-density plasma for ionized metal deposition capable of exciting a plasma wave |
US7335282B2 (en) | 1999-02-12 | 2008-02-26 | Jianming Fu | Sputtering using an unbalanced magnetron |
JP2002536556A (en) * | 1999-02-12 | 2002-10-29 | アプライド マテリアルズ インコーポレイテッド | High density plasma source for ionized metal deposition |
US6497802B2 (en) | 1999-02-12 | 2002-12-24 | Applied Materials, Inc. | Self ionized plasma sputtering |
US6440282B1 (en) | 1999-07-06 | 2002-08-27 | Applied Materials, Inc. | Sputtering reactor and method of using an unbalanced magnetron |
JP2001140070A (en) * | 1999-08-12 | 2001-05-22 | Applied Materials Inc | High density plasma source for ionized metal deposition |
US6358376B1 (en) * | 2000-07-10 | 2002-03-19 | Applied Materials, Inc. | Biased shield in a magnetron sputter reactor |
US6663754B2 (en) | 2001-04-13 | 2003-12-16 | Applied Materials, Inc. | Tubular magnet as center pole in unbalanced sputtering magnetron |
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