JPS63109165A - Magnetron type sputtering device - Google Patents

Magnetron type sputtering device

Info

Publication number
JPS63109165A
JPS63109165A JP25610786A JP25610786A JPS63109165A JP S63109165 A JPS63109165 A JP S63109165A JP 25610786 A JP25610786 A JP 25610786A JP 25610786 A JP25610786 A JP 25610786A JP S63109165 A JPS63109165 A JP S63109165A
Authority
JP
Japan
Prior art keywords
target
magnet
sputtering device
type sputtering
magnetron type
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP25610786A
Other languages
Japanese (ja)
Inventor
Matsutomo Mori
森 松倫
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP25610786A priority Critical patent/JPS63109165A/en
Publication of JPS63109165A publication Critical patent/JPS63109165A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To promote both the increase of Ar ion and the improvement of dispersion thereof and to enhance the coefficient of effective utilization of a target by increasing a magnet provided on the rear surface of the target to a plurality of pieces in a magnetron sputtering device. CONSTITUTION:In a magnetron sputtering device wherein both a base plate 8 fitted to an anode 9 and a target 2 provided with magnets to the rear surface thereof and impressed with negative voltage are oppositely arranged, the number of the magnet 1 is regulated to at least three pieces or more. Since secondary electrons 4 are subjected to cycloidal motion on the target 2 by means of lines 3 of magnetic force having component parallel to the surface of the target 2, the ionization of Ar is promoted and Ar ions are allowed to collide against the target 2 as a cathode to sputter the target 2 and a thin film is formed on the base plate 8 by depositing the target thereon. Magnetic fields parallel to the surface of the target are increased because the many magnet 1 and the number of Ar ion is increased with dispersion thereof uniformized and the errosion part is windened; thereby the coefficient of utilization is enhanced.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はマグネトロン型スパッタ装置の改良に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to improvements in magnetron type sputtering equipment.

〔従来の技術〕[Conventional technology]

従来のマグネトロン型スパッタ装置は、第3図に示すよ
うに、裏面側に磁石1を有するターゲット2に対向して
配設された陽極を兼ねる基板ホルダ9に基板8を取付け
て、ターゲラ1゛2がらなたき出された2次電子の運動
によりArイオン化を促進させ、形成されたArイオン
をターゲット2に衝突させてターゲツト材をスパッタさ
せ、基板S上に堆積させて薄膜を形成するものである。
As shown in FIG. 3, in a conventional magnetron type sputtering apparatus, a substrate 8 is attached to a substrate holder 9 which also serves as an anode and is disposed facing a target 2 having a magnet 1 on the back side. Ar ionization is promoted by the movement of the secondary electrons ejected from the glass, and the formed Ar ions collide with the target 2 to sputter the target material and deposit it on the substrate S to form a thin film. .

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

上述した従来のマグネトロン型スパッタ装置では、円筒
状の磁石が2個しか用いられていないのでターゲット表
面から出た電子を拘束するのに必要なターゲット表面に
平行な磁力線が少ないという欠点がある。しかも、電子
を拘束できるというターゲット表面に平行な磁力線が限
られている為、ターゲットの侵食部分が一部分のみとな
り、ターゲットの有効利用率が低いという欠点ある。
The conventional magnetron sputtering apparatus described above uses only two cylindrical magnets, and therefore has the disadvantage that there are few lines of magnetic force parallel to the target surface necessary to restrain electrons emitted from the target surface. Moreover, since there are only a limited number of magnetic lines of force parallel to the target surface that can bind electrons, only a portion of the target is eroded, resulting in a low effective utilization rate of the target.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は、裏面側に磁石を設置したターゲットに対向し
て設けた陽極上に配設した基板上にターゲットからスパ
ッタされた粒子を堆積させるマグネトロン型スパッタ装
置において、ターゲットの有効利用率を高める為に3個
以上のマグネットをターゲット裏面に配設することを特
徴とする。
The present invention is aimed at increasing the effective utilization rate of a target in a magnetron type sputtering device in which particles sputtered from a target are deposited on a substrate placed on an anode provided opposite to a target with a magnet installed on the back side. The target is characterized in that three or more magnets are arranged on the back side of the target.

〔実施例〕〔Example〕

次に本発明について図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.

第1図は本発明の一実施例を示す概略構成図である。負
電圧をかけられたターゲット2から放出された2次電子
4は磁石1の作る磁界3の影響を受けて運動する。特に
ターゲット2の表面と平行な成分を持つ磁力線は2次電
子4をターゲット2上でサイクロイド運動される為、A
rのイオン化を促進させ、Arイオンを作り出す。Ar
イオンは陰極であるターゲット2に衝突してターゲツト
材をスパッタさせる。その結果、ターゲツト材が半導体
などの基板8上に堆積し、薄膜を形成する。
FIG. 1 is a schematic diagram showing an embodiment of the present invention. Secondary electrons 4 emitted from the target 2 to which a negative voltage is applied move under the influence of the magnetic field 3 created by the magnet 1. In particular, the magnetic field lines with components parallel to the surface of the target 2 cause the secondary electrons 4 to move cycloidally on the target 2, so A
The ionization of r is promoted to produce Ar ions. Ar
The ions collide with target 2, which is a cathode, and sputter target material. As a result, the target material is deposited on the substrate 8, such as a semiconductor, to form a thin film.

従って、ターゲット2に衝突するArイオンが多ければ
多い程、ターゲットは侵食され、しかもA1−イオンの
分布が均一なほどターゲットの有効利用率は上昇する。
Therefore, the more Ar ions that collide with the target 2, the more the target is eroded, and the more uniform the distribution of A1- ions, the higher the effective utilization rate of the target.

第2図はターゲット、磁石部分の横断面図(a)と縦断
面図(b)を示している。この例は4個のマグネットを
有する場合を示している。本発明では3個以上の磁石を
ターゲラI・裏面に設置するので、ターゲット表面に平
行な磁界を増加し、Arイオンを増加させると共に、分
布も均一となる。
FIG. 2 shows a cross-sectional view (a) and a vertical cross-sectional view (b) of the target and magnet portion. This example shows a case with four magnets. In the present invention, three or more magnets are installed on the back surface of Targetera I, so that the magnetic field parallel to the target surface is increased, the Ar ions are increased, and the distribution becomes uniform.

その結果、ターゲットの有効利用率は一ヒ昇する。As a result, the effective utilization rate of the target will increase by a bit.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、マグネ1−ロン型スパッ
タ装置において、ターゲットの裏面にある磁石を従来よ
り増加させることにより、Arイオンの増大1分布の改
善を促進させ、その結果、ターゲットの有効利用率を」
−Hさせる効果がある。
As explained above, the present invention promotes an improvement in the distribution of Ar ions by increasing the number of magnets on the back surface of the target in a magnetron type sputtering apparatus compared to the conventional one, and as a result, the effectiveness of the target is increased. "Utilization rate"
-It has the effect of making you H.

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

第1図は本発明の一実施例の概略構成図、第2図(a>
、(b)はそれぞれ第1図のターゲットと磁石部分の横
断面図および縦断面図、第3図は従来のマグネトロン型
スパッタ装置の概略構成図である。 1・・・磁石、2・・・ターゲラI・、3・・・磁力線
、4・・・2次電子、7・・電源、8・・・基板、9・
・・陽極(基板ホルダー)、10・・・エロージョン。
FIG. 1 is a schematic configuration diagram of an embodiment of the present invention, and FIG. 2 (a>
, (b) are a cross-sectional view and a vertical cross-sectional view of the target and magnet portions of FIG. 1, respectively, and FIG. 3 is a schematic diagram of a conventional magnetron type sputtering apparatus. DESCRIPTION OF SYMBOLS 1...Magnet, 2...Tagera I, 3...Magnetic field lines, 4...Secondary electrons, 7...Power source, 8...Substrate, 9...
... Anode (substrate holder), 10... Erosion.

Claims (1)

【特許請求の範囲】[Claims] 裏面側に磁石を有するターゲットに対向して陽極を配設
し、この陽極に基板を取付け、ターゲット材をスパッタ
させ基板上に堆積させるマグネトロン型スパッタ装置に
おいて、ターゲット裏面に3個以上のマグネットを配置
することを特徴とするマグネトロン型スパッタ装置。
In a magnetron type sputtering device, an anode is placed facing a target that has a magnet on the back side, a substrate is attached to the anode, and target material is sputtered and deposited on the substrate. Three or more magnets are placed on the back side of the target. A magnetron type sputtering device characterized by:
JP25610786A 1986-10-27 1986-10-27 Magnetron type sputtering device Pending JPS63109165A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25610786A JPS63109165A (en) 1986-10-27 1986-10-27 Magnetron type sputtering device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25610786A JPS63109165A (en) 1986-10-27 1986-10-27 Magnetron type sputtering device

Publications (1)

Publication Number Publication Date
JPS63109165A true JPS63109165A (en) 1988-05-13

Family

ID=17287986

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25610786A Pending JPS63109165A (en) 1986-10-27 1986-10-27 Magnetron type sputtering device

Country Status (1)

Country Link
JP (1) JPS63109165A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2001077405A1 (en) * 2000-04-10 2001-10-18 Kurt J. Lesker Company Magnetron sputtering source with improved target utilization and deposition rate

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2001077405A1 (en) * 2000-04-10 2001-10-18 Kurt J. Lesker Company Magnetron sputtering source with improved target utilization and deposition rate

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