TW200538568A - Sputtering apparatus - Google Patents

Sputtering apparatus Download PDF

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Publication number
TW200538568A
TW200538568A TW094105312A TW94105312A TW200538568A TW 200538568 A TW200538568 A TW 200538568A TW 094105312 A TW094105312 A TW 094105312A TW 94105312 A TW94105312 A TW 94105312A TW 200538568 A TW200538568 A TW 200538568A
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Taiwan
Prior art keywords
targets
magnetic field
film
forming means
target
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TW094105312A
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Chinese (zh)
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TWI375729B (en
Inventor
Makoto Arai
Yuichi Oishi
Satoru Ishibashi
Takashi Komatsu
Noriaki Tani
Junya Kiyota
Atsushi Ota
Kyuzo Nakamura
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Ulvac Inc
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Publication of TWI375729B publication Critical patent/TWI375729B/en

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    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
    • C23C14/35Sputtering by application of a magnetic field, e.g. magnetron sputtering
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
    • C23C14/3464Sputtering using more than one target

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  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • Mechanical Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Physical Vapour Deposition (AREA)

Abstract

The present invention provides a film-forming apparatus for forming a film with uniform thickness distribution, by reducing overdischarge and a non-eroded portion. The film-forming apparatus 1 has a plurality of targets 31a to 31f, and alternating voltages with different polarities are applied to the different targets 31a to 31f from the same alternating power source. When one set of targets 31a, 31c and 31e are set to a negative potential, the other set of targets 31b, 31d and 31f are set to a positive potential and work as the anodes, so that there is no need to arrange the anode between the adjacent targets out of the targets 31a to 31f. Because of arranging nothing between the adjacent targets out of the targets 31a to 31f, the film-forming apparatus can shorten the distance (s) among the targets 31a to 31f, and because of reducing a ratio of the area which does not emit sputtered particles, with respect to areas in which the targets 31a to 31f are arranged, the film-forming apparatus makes the sputtered particles uniformly arrive at the substrate 5 and the film thickness distribution uniform.

Description

200538568 (1) 九、發明說明 【發明所屬之技術領域】 本發明係關於一種濺射裝置。 【先前技術】 第8圖的元件符號1 01係表示習知技術的成膜裝置。200538568 (1) IX. Description of the invention [Technical field to which the invention belongs] The present invention relates to a sputtering device. [Prior Art] The reference numeral 1 01 in FIG. 8 indicates a film forming apparatus of a conventional technique.

成膜裝置1 〇 1係具有:真空槽1 〇 2以及配置於真空槽 102內部的複數個靶材131a至13 le。 各靶材1 3 1 a至1 3 1 e係呈細長板狀,在濺射面朝向配 置於真空槽1 02內部的基板1 〇5的狀態下,間隔一定以上 的間隔而相互平行配置。 在一面藉由真空排氣系統1 1 2對真空槽1 02內部進行 真空排氣,一面由氣體供給系統1 1 3將濺射氣體導入真空 槽1 02內部,而在真空槽1 02內部形成成膜環境氣體之狀 態下,起動連接有電極1 3 5 a至1 3 5 e之電源1 1 7 a至 1 1 7 e,且當在將真空槽1 0 2與基板1 0 5置於接地電位的狀 態下對各靶材1 3 1 a至1 3 1 e施加交流電壓時,使靶材 1 3 1 a至1 3 1 e的表面受到濺射。 當同時濺射複數個靶材1 3 1 a至1 3 1 e時,將置於接地 電位的屏蔽(shield ) 1 1 1僅配置在靶材1 3 la至1 3 1 e的 周邊部時,電漿雖會偏向配置有屏蔽1 1 1的方向,但是由 於在該成膜裝置1 0 1中,在靶材1 3 1 a至1 3 1 e之間亦配置 有置於接地電位的屏蔽1 1 1,因此電漿不會偏向,而使各 靶材1 3 1 a至:m e均勻受到濺射。 -5- 200538568 (2) 於靶材〗3 I a至1 3 1 e之濺射面的相反側,沿著靶材 13 1a至131e的長邊方向配置有細長的磁場形成手段140a 至140e。磁場形成手段140a至140e的寬度比靶材131a 至1 3 1 e的寬度短,藉由未圖示的移動手段,可由靶材 1 3 1 a至1 3 1 e的寬度方向的一端至另一端往返移動。 因此,由磁場形成手段1 4 0 a至1 4 0 e所形成的磁場亦 於靶材1 3 1 a至1 3 1 e表面移動,因此,電漿密度較高的部 分於靶材1 3 1 a至1 3 1 e表面移動,而使靶材1 3 1 a至1 3 1 e 較寬區域受到濺射。 在使用複數個靶材的成膜裝置中,由於靶材數較多之 故,而使濺射粒子釋出在較寬區域,因此,可在大面積的 基板105進行成膜處理。 然而,習知成膜裝置具有以下所述之問題點。首先, 第一,由於從屏蔽11 1所位之處並未釋出濺射粒子,因 此,基板1 0 5表面之位於屏蔽1 1 1上的部分與位於靶材 131a至131e上的部分會發生膜厚分布及膜質分布不均勻 的情形。 此外,如上所述,一面使磁場形成手段1 4 0 a至1 4 0 e 移動,一面對靶材1 3 1 a至1 3 1 e施加交流電壓時,隨著磁 場形成手段14〇a至140e的移動,電漿密度較高的部分亦 隨之移動。 因此,與濺射氣體一起導入如氧氣的反應性氣體而進 行濺射時,當電漿密度較高的部分發生移動時,會在濺射 面的電漿密度變小的部分,靶材材料與反應性氣體發生反 -6- 200538568 (3) 而成爲異常放電的 應而形成反應物的膜(例如氧化膜) 原因。 若將磁場形成手段1 4 0 a至1 4 0 e予以固定而不移動地 進行濺射,電漿密度較高的部分雖不會發生移動的情形, 但在?巴材1 3 1 a至1 3 1 e內(尤其是靶材1 3 ] a至1 3 1 e之寬 度方向的中央部分)會產生非侵蝕部,該非侵蝕部即成爲 異常放電的原因,此外,亦造成非侵蝕部發生剝離而產生 微粒(particle)的原因。 [專利文獻1]日本專利特表2002-508447號公報 [專利文獻2 ]日本專利特開平1 1 - 2 4 1 1 5 9號公報 [專利文獻3]日本專利特開平9-13160號公報 【發明內容】 (發明所欲解決之課題) 本發明係爲解決上述習知技術的問題點而硏創者,目 的在於提供一種可形成侵蝕區域廣、不會發生異常放電、 膜厚分布均勻之薄膜的成膜裝置。 (解決課題之手段) 爲解決上述課題,申請專利範圍第1項之發明係一種 成膜裝置,係具有:真空槽;複數個具有長邊方向的板狀 靶材;以及對於前述靶材施加交流電壓的交流電源,於前 述複數個靶材之中,由相同的交流電源施加極性不同的交 流電壓至不同的靶材,前述複數個靶材係在濺射面朝向相 200538568 (4) 同方向的狀態下,將相鄰的前述靶材之長邊方向的側面配 置成僅透過前述真空槽中的環境氣體而相互直接對向。 申請專利範圍第2項的發明係如申請專利範圍第1項 之成膜裝置,其中,相互對向的前述側面彼此間之距離係 設爲1 m m以上、1 0 m m以下。 申請專利範圍第3項的發明係如申請專利範圍第1項 1 或第2項之成膜裝置,其中,前述交流電源部的頻率係爲 • 1kHz 以上、100kHz 以下。 申請專利範圍第4項之發明係一種成膜裝置,係具 有:真空槽;以及配置於前述真空槽內部之複數個細長板 狀靶材,前述各靶材係相互平行配置成長邊方向的側面彼 此呈相對向的狀態,在前述各靶材的正背面位置,沿著前 述靶材的長邊方向分別配置有細長的磁場形成手段,在比 前述靶材的正背面位置還外側之配置有前述磁場形成手段 I 的區域外側,係沿著前述靶材的長邊方向配置有細長的輔 • 助磁場形成手段。 申請專利範圍第5項之發明係如申請專利範圍第4項 之成膜裝置,其中,前述各磁場形成手段係具有複數個磁 鐵,前述複數個磁鐵之中,與前述輔助磁場形成手段相鄰 配置之磁鐵之朝向前述靶材側的面的磁極,係設定成與前 述輔助磁場形成手段之朝向前述靶材側的面的磁極相同的 極性。 申請專利範圍第6項之發明係如申請專利範圍第4項 或第5項之成膜裝置,其中,具有移動手段,用於使前述 200538568 (5) 磁場形成手段與前述輔助磁場形成手段相對於前述靶材作 相對移動。 本發明係如上所構成,在相鄰靶材彼此之間並未配置 接地電極或絕緣物,因此,當對真空槽內部進行真空排氣 時,在相鄰靶材之長邊方向的側面相對向的區域亦形成真 空環境氣體,該真空環境氣體的寬度係與側面彼此間之距 > 離相等。 φ 未配置任何構件之故,而可使側面彼此間之距離縮小 爲1mm以上、10mm以下,因此未釋出濺射粒子的區域會 變窄,因而使得到達基板的濺射粒子量的分布呈均勻狀 態。 若使磁場形成手段的寬度與靶材寬度大致相等,即使 在未使磁場形成手段移動的情況下進行濺射,亦可提高靶 材整個表面區域的電漿密度,但是如上所述當靶材彼此間 > 的間隔較短時,磁場形成手段彼此間的間隔亦會變短。將 • 複數台磁場形成手段近接配置時,由於相互鄰接的磁場形 成手段彼此的磁場千擾,會使磁場失去平衡。尤其是,使 用交流電源來進行濺射時,由於形成一對的陰極(靶材) 彼此間的放電阻抗(impedance )會不同,因此會造成膜 厚、膜質分布惡化,更甚者,會產生形成一對的陰極彼此 的靶材使用效率惡化的問題。 本發明的成膜裝置中,在比配置靶材的區域還外側之 配置在最外側的磁場形成手段的附近位置具有輔助磁場形 成手段,藉由該輔助磁場形成手段,可使接近磁場形成手 -9- 200538568 (6) 段時的磁場干擾變得較爲緩和,因此,磁場強度不會失去 平衡,而在各靶材的表面使磁通密度分布均勻。 一面使磁場形成手段相對於靶材作相對移動,一面進 行濺射時,由於磁力線遠離,而使電漿密度變少的部分並 不會受到濺射,使得在靶材表面形成與反應性氣體進行反 應的反應物(例如氧化物),該反應物雖會形成異常放電 或微粒(particle )的原因,但是如上所述,在本發明 • 中,並不需要使磁場形成手段移動,即可在相對於靶材爲 固定的狀態下來進行濺射,所以不會發生異常放電。 (發明的效果) 若使用本發明的成膜裝置,即使成膜在大型基板時, 亦可獲得膜厚分布及膜質分布佳的膜。此外,由於不需設 置接地屏蔽(earth shield )零件,因而使得來自接地屏蔽 1 零件部分的微粒減少。再者,與習知裝置相較之下,由於 # 不需設置接地屏蔽零件、磁路(magnetic circuit )的搖動 機構、電源之異常放電防止機構,故可減少零件數量,削 減成本,且可改善裝置維護性。 【實施方式】 第1圖的元件符號1係表示本發明之成膜裝置之一 例,該成膜裝置1係具有:真空槽2 ;配置在真空槽2內 部的基板保持具(s u b s tr a te h 0 1 d e r ) 4 ;以及配置在與真 空槽2內部的基板保持具4相對向位置的濺射源3。濺射 -10-The film forming apparatus 101 includes a vacuum tank 102 and a plurality of targets 131a to 13e arranged inside the vacuum tank 102. Each of the targets 1 3 1 a to 1 3 1 e has an elongated plate shape, and is arranged in parallel with each other at a certain interval or more with the sputtering surface facing the substrate 1 05 arranged inside the vacuum chamber 102. The inside of the vacuum tank 102 is evacuated by the vacuum exhaust system 1 12 on the one side, and the sputtering gas is introduced into the vacuum tank 10 02 by the gas supply system 1 1 3 while being formed inside the vacuum tank 102 In the state of the membrane ambient gas, start the power supply 1 1 7 a to 1 3 5 e connected to the electrodes 1 3 5 a to 1 3 5 e, and when the vacuum tank 1 2 and the substrate 1 0 5 are placed at the ground potential When an AC voltage is applied to each of the targets 1 3 1 a to 1 3 1 e in a state of being exposed, the surfaces of the targets 1 3 1 a to 1 3 1 e are sputtered. When a plurality of targets 1 3 1 a to 1 3 1 e are sputtered at the same time, a shield 1 1 1 placed at the ground potential is disposed only at the periphery of the targets 1 3 la to 1 3 1 e. Although the plasma will be biased to the direction where the shield 1 1 1 is arranged, the shield 1 placed at the ground potential is also arranged between the targets 1 3 1 a to 1 3 1 e in the film forming apparatus 1 0 1. Since the plasma is not biased, each target 1 3 1 a to: me is uniformly sputtered. -5- 200538568 (2) On the opposite side of the sputtering surface of the target material 3 I a to 1 3 1 e, elongated magnetic field forming means 140a to 140e are arranged along the long side direction of the target material 13 1a to 131e. The widths of the magnetic field forming means 140a to 140e are shorter than the widths of the targets 131a to 1 3 1e. The moving means (not shown) can be used to move the ends of the targets 1 3 1 a to 1 3 1 e in the width direction to the other end. Move back and forth. Therefore, the magnetic field formed by the magnetic field forming means 1 4 0 a to 1 4 0 e also moves on the surface of the target 1 3 1 a to 1 3 1 e. Therefore, the higher plasma density is in the target 1 3 1 The surface of a to 1 3 1 e moves, and a wide area of the targets 1 3 1 a to 1 3 1 e is sputtered. In a film forming apparatus using a plurality of targets, since the number of targets is large, the sputtered particles are released in a wide area. Therefore, a film formation process can be performed on a large-area substrate 105. However, the conventional film forming apparatus has the problems described below. First, first, since sputter particles are not released from the position where the shield 11 1 is located, a portion of the surface of the substrate 105 located on the shield 1 1 1 and a portion located on the targets 131 a to 131 e occur. Film thickness distribution and uneven film quality distribution. In addition, as described above, when the magnetic field forming means 1 40 a to 1 4 0 e is moved, and when an AC voltage is applied to the target 1 3 1 a to 1 3 1 e, the magnetic field forming means 14 0a to With the movement of 140e, the higher density part of the plasma moves with it. Therefore, when a reactive gas such as oxygen is introduced together with the sputtering gas to perform sputtering, when the plasma density portion moves, the plasma density on the sputtering surface becomes smaller, and the target material and the Reactive gas is anti-6-200538568 (3) The cause of abnormal discharge and the formation of a film (such as an oxide film) of reactants. If the magnetic field forming means 1 40 a to 1 40 e is fixed and sputtered without moving, the high plasma density part does not move, but what happens? There is a non-eroded part in the base material 1 3 1 a to 1 3 1 e (especially in the central part in the width direction of the target 1 3] a to 1 3 1 e). This non-eroded part becomes the cause of abnormal discharge. In addition, It also causes the non-eroded part to peel off and cause particles. [Patent Document 1] Japanese Patent Publication No. 2002-508447 [Patent Literature 2] Japanese Patent Publication No. 1 1-2 4 1 1 5 9 [Patent Literature 3] Japanese Patent Publication No. 9-13160 [Invention Contents] (Problems to be Solved by the Invention) The present invention was created in order to solve the problems of the above-mentioned conventional technologies, and aims to provide a thin film that can form a wide erosion area without abnormal discharge and uniform film thickness distribution. Film forming device. (Means for solving problems) In order to solve the above-mentioned problems, the first invention of the patent application scope is a film-forming device having: a vacuum tank; a plurality of plate-shaped targets having a long-side direction; and applying AC to the aforementioned targets The AC power source of voltage is applied to the different target materials by the same AC power source among the plurality of target materials. The target materials are on the sputtering surface facing the same direction. 200538568 (4) In the state, the side surfaces in the longitudinal direction of the adjacent targets are arranged so as to directly face each other only through the ambient gas in the vacuum tank. The invention according to the second patent application scope is the film-forming device according to the first patent application scope, wherein the distance between the side surfaces facing each other is set to be 1 m m or more and 10 m m or less. The invention with the scope of patent application No. 3 is the film-forming device of the scope of patent application No. 1 or 2, wherein the frequency of the aforementioned AC power supply unit is 1 kHz or more and 100 kHz or less. The invention of claim 4 is a film-forming device, comprising: a vacuum tank; and a plurality of elongated plate-shaped targets arranged inside the vacuum tank, and the targets are arranged parallel to each other in the direction of the growth direction. In a facing state, elongated magnetic field forming means are arranged along the longitudinal direction of the target at the front and back positions of the targets, and the magnetic field is arranged outside the front and back positions of the targets. Outside the area of the forming means I, an elongated auxiliary magnetic field forming means is arranged along the longitudinal direction of the target. The invention of claim 5 is the film-forming device of claim 4, wherein each of the magnetic field forming means has a plurality of magnets, and among the plurality of magnets, it is disposed adjacent to the auxiliary magnetic field forming means. The magnetic pole of the surface of the magnet facing the target side is set to have the same polarity as the magnetic pole of the surface facing the target side of the auxiliary magnetic field forming means. The invention claimed in item 6 of the patent application is a film-forming device such as the item 4 or 5 in the patent application, which has a moving means for making the aforementioned 200538568 (5) magnetic field forming means and the auxiliary magnetic field forming means opposite to The target is moved relatively. The present invention is constituted as described above, and no ground electrode or insulator is arranged between adjacent targets. Therefore, when the inside of the vacuum chamber is evacuated, the sides of the adjacent targets in the long side direction face each other. A vacuum ambient gas is also formed in the region of the vacuum atmosphere, and the width of the vacuum ambient gas is equal to the distance > distance between the sides. φ Because no member is arranged, the distance between the sides can be reduced to 1 mm or more and 10 mm or less, so the area where the sputter particles are not released will be narrowed, so that the distribution of the amount of sputter particles reaching the substrate is uniform. status. If the width of the magnetic field forming means is approximately equal to the width of the target, even if sputtering is performed without moving the magnetic field forming means, the plasma density of the entire surface area of the target can be increased. When the interval between intervals is shorter, the interval between the magnetic field forming means becomes shorter. • When multiple magnetic field forming means are arranged close to each other, the magnetic fields will be out of balance due to the magnetic field interference of adjacent magnetic field forming means. In particular, when an AC power source is used for sputtering, the formation of a pair of cathodes (target materials) will have different discharge impedances, which will result in deterioration of film thickness and film quality distribution, and furthermore, formation of There is a problem that the target use efficiency of a pair of cathodes deteriorates. In the film forming apparatus of the present invention, an auxiliary magnetic field forming means is provided near the outermost magnetic field forming means outside the region where the target is disposed, and the auxiliary magnetic field forming means can be used to form a hand near the magnetic field- The magnetic field interference at 9-200538568 (6) becomes more moderate, so the magnetic field intensity will not lose balance, and the magnetic flux density distribution will be uniform on the surface of each target. While the magnetic field forming means is relatively moved relative to the target, while sputtering is performed, because the magnetic lines of force are far away, the part with a reduced plasma density is not subject to sputtering, so that the formation of the target surface with the reactive gas occurs. The reactants (such as oxides) of the reaction may cause abnormal discharges or particles, but as described above, in the present invention, it is not necessary to move the magnetic field forming means, and the relative Since sputtering is performed with the target in a fixed state, abnormal discharge does not occur. (Effects of the Invention) With the film forming apparatus of the present invention, a film having a good film thickness distribution and film quality distribution can be obtained even when a film is formed on a large substrate. In addition, since there is no need to provide a ground shield part, particles from the part of the ground shield 1 are reduced. In addition, compared with the conventional device, # does not need to be provided with a ground shielding component, a magnetic circuit shaking mechanism, and an abnormal discharge prevention mechanism for the power supply, so the number of parts can be reduced, costs can be reduced, and improvements can be made. Device maintainability. [Embodiment] The reference numeral 1 in FIG. 1 shows an example of a film forming apparatus according to the present invention. The film forming apparatus 1 includes: a vacuum tank 2; and a substrate holder (subs tr a te h) disposed inside the vacuum tank 2. 0 1 der) 4; and a sputtering source 3 disposed at a position facing the substrate holder 4 inside the vacuum chamber 2. Sputtering -10-

200538568 (7) 源3係具有複數個濺射部3 0 a至3 0 f ◦各濺射部 3 〇 f係分別具有板狀靶材3 1 a至3 1 f,當將各靶材 3 1 f受到濺射的面作爲濺射面時,各靶材3 1 a至3 置成使各濺射面位在相同平面上。 各靶材3 1 a至3 1 f係成形爲具有長邊方向的細 各濶射面亦形成具有長邊方向的細長狀。各靶材 3 1 f係分別爲相同形狀,將濺射面之長邊方向的邊 (側面)以相互隔著預定間隔的方式平行配置。 相鄰的靶材3 1 a至3 1 f的側面彼此係形成爲僅 定距離,因此,相鄰的靶材3 1 a至3 1 f的側面係 行。在本發明中,靶材3 1 a至3 1 f間並未配置電 蔽,而靶材3 1 a至3 1 f的側面彼此係直接相面對。 在各靶材3 1 a至3 1 f的背面,係將與各靶材 3 1 f相同寬度、相同長度的電極3 5 a至3 5 f密接安 會從靶材3 1 a至3 1 f的外周突出。 在真空槽2外部配置有交流電源17a至17c, 電源17a至17c的2個端子之中,一方的端子係與 2個電極35a至35f中之一方的電極35a、35c、3ί 接,另一方的端子則係連接於另一方的電極3 5 b、 35f 〇 各交流電源1 7 a至1 7 c的2個端子係形成輸出 同極性的電壓,靶材3 1 a至3 1 f係密接安裝於電極 3 5 f,所以對於相鄰2個靶材3 1 a至3 1 f係由交流霄 至1 7 c施加極性互相不同的交流電壓。因此,形成 30a至 31a至 1 f係配 長狀, 31a至 緣部分 間隔一 形成平 極或屏 31a至 裝成不 各交流 相鄰之 相連 35d、 正負不 3 5 a至 ,源 1 7 a 在彼此 - 11 -200538568 (7) The source 3 series has a plurality of sputtering portions 3 0 a to 30 f. Each sputtering portion 3 0f has a plate-shaped target 3 1 a to 3 1 f. When each target 3 1 When the surface subjected to sputtering is used as the sputtering surface, the targets 3 1 a to 3 are placed so that the sputtering surfaces are positioned on the same plane. Each of the targets 3 1 a to 3 1 f is formed into a thin shape having a long side direction, and each projecting surface is also formed into an elongated shape having a long side direction. Each of the targets 3 1 f has the same shape, and the sides (side surfaces) in the longitudinal direction of the sputtering surface are arranged in parallel with a predetermined interval therebetween. The sides of the adjacent targets 3 1 a to 3 1 f are formed at a certain distance from each other, and therefore, the sides of the adjacent targets 3 1 a to 3 1 f are aligned. In the present invention, no shielding is provided between the targets 3 1 a to 3 1 f, and the sides of the targets 3 1 a to 3 1 f face each other directly. On the back of each target 3 1 a to 3 1 f, electrodes 3 5 a to 3 5 f with the same width and the same length as each target 3 1 f are tightly connected from the target 3 1 a to 3 1 f. The periphery is prominent. Among the two terminals of the AC power supply 17a to 17c and the power supply 17a to 17c, one of the terminals is connected to one of the electrodes 35a, 35c, and 3f of the two electrodes 35a to 35f. The terminals are connected to the other electrode 3 5 b, 35f 〇 2 terminals of each AC power supply 17 a to 17 c form the output voltage of the same polarity, and the target materials 3 1 a to 3 1 f are closely mounted on Since the electrode 3 5 f is applied to two adjacent targets 3 1 a to 3 1 f, AC voltages of mutually different polarities are applied from AC to 17 c. Therefore, 30a to 31a to 1f are formed in a long shape, and 31a to the edge portion is formed as a flat pole or a screen 31a to be connected to each other adjacently for 35d, plus or minus 3 5a to, source 1 7a in Each other-11-

200538568 (δ) 相鄰接之祀材J 1 a至3 1 f之中,一方置於正電位 方則置於負電位的狀態。 在電極3 5 a至3 5 f之與靶材3 1 a至3 1 f相反側 安裝有絕緣板3 3 a至3 3 f,靶材3 1 a至3 1 f及電極 35f係形成與後述之磁場形成手段40a至40f或其 絕緣。 在電極3 5 a至3 5 f之與靶材3 1 a至3 1 f相反側 配置有磁場形成手段4 0 a至4 0 f。參照第2圖,各 成手段4 0 a至4 0 f係分別具有:具有外周與靶材 3 1 f的外周大致相等之尺寸的細長環狀磁鐵42a至 以及比環狀磁鐵42a至42f的長度還短的棒狀磁鐵 43f 〇 各環狀磁鐵42a至42f係在相對應的1個靶材 3 1 f的正背面位置,配置成與靶材3 1 a至3 1 f之長200538568 (δ) Among the adjacent materials J 1 a to 3 1 f, one is placed at a positive potential and the other is placed at a negative potential. An insulating plate 3 3 a to 3 3 f is mounted on the opposite side of the electrodes 3 5 a to 3 5 f from the target 3 1 a to 3 1 f. The target 3 1 a to 3 1 f and the electrode 35f are formed and described later. The magnetic field forming means 40a to 40f or their insulation. Magnetic fields forming means 4 0 a to 4 0 f are arranged on the electrodes 3 5 a to 3 5 f on the opposite sides of the targets 3 1 a to 3 1 f. Referring to FIG. 2, each of the forming means 40 a to 40 f has an elongated ring magnet 42 a having a size substantially equal to the outer periphery of the target 3 1 f and a length longer than the ring magnets 42 a to 42 f. The short rod-shaped magnet 43f. Each ring magnet 42a to 42f is located at the front and back positions of the corresponding target 3 1 f, and is arranged to be as long as the target 3 1 a to 3 1 f.

I 平行。如上所述,靶材3 1 a至3 1 f係以預定間隔 Φ 置,所以環狀磁鐵42a至42f係形成以隔著與靶材 3 1 f相同間隔的方式而配置的狀態。 棒狀磁鐵43a至43f係在環狀磁鐵42a至42f 內部,沿著靶材3 1 a至3 1 f的長邊方向予以配置。 棒狀磁鐵43a至43f之長邊方向的側面兩側係形成 環狀磁鐵42a至42f的狀態。 磁場形成手段40a至40f的磁鐵中,將配置在 磁鐵(環狀磁鐵)設爲第一磁鐵42a至42f,配置 磁鐵42a至4 2f之間的磁鐡(棒狀磁鐵)設爲第 ,另一 的面係 3 5 a至 他構件 的面係 磁場形 31a至 42f ; 43a至 31a至 邊方向 平行配 31a至 的環形 因此, 配置有 兩側的 在第一 二磁鐵 - 12- 200538568 Ο) 43a至43f時,第一^磁鐵42a至42f、弟—·磁鐵43a至43f 的磁極係位在厚度方向的兩端,亦即位在表面側與背面 側,當將朝向靶材3 1 a至3 1 f側的面設爲表面時,在第一 磁鐵4 2 a至4 2 f、第二磁鐵4 3 a至4 3 f的背面側係密接有 板狀磁軛4 1 a至4 1 f。 因此,在第一磁鐵42&至42f、第二磁鐵43a至43f > 的背面側的磁極之間產生的磁力線係形成通過磁軛4 1 a至 # 4 1 f的內部。磁軛4 1 a至4 1 f的平面形狀係與第一磁鐵 42a至42f之環形的外周相等,第一磁鐵42a至42f係配 置成不會從磁轭4 1 a至4 1 f的邊緣突出。如上所述,第一 磁鐵42a至42f的形狀係與靶材31a至3 If大致相等,所 以磁場形成手段40a至40f的平面形狀亦與靶材31a至 3 1 f大致相等。 在此’各磁場形成手段40a至40f係配置在相對應的 k 1個靶材3 1 a至3 1 f的正背面位置,所以各磁場形成手段 Φ 4〇3至40f不會從靶材31a至31f的外周突出,各磁場形 成手段40a至40f並不會配置成跨越2個靶材31a至 3 1卜 第一磁鐵42a至42f之表面側之磁極的磁性爲N極 時’第二磁鐵43a至43f之表面側之磁極的磁性則爲s 極’當第一磁鐵42a至42f之表面側之磁極的磁性爲S極 時’第二磁鐵43a至43f之表面側之磁極的磁性則爲N 極,因此’第一磁鐵42a至42f的表面與第二磁鐵43a至 43f的表面之間係形成有通過電極35a至35f的磁力線。 -13- 200538568 (10) 各電極3 5 a至3 5 f內部之位於第二磁鐵4 3 a至4 3 f上 的位置係分別配置有由磁導性(p e r m e a b i 1 i t y )材料(在 此係純度99.8%的純鐵)構成的磁性體36a至3 6f,且通 過電極35a至3 5f的磁力線係藉由該磁性體36a至3 6f而 被吸引到靶材3 1 a至3 1 f側,且通過靶材3 1 a至3 1 f的表 面。I parallel. As described above, the targets 3 1 a to 3 1 f are arranged at a predetermined interval Φ. Therefore, the ring magnets 42 a to 42 f are in a state of being arranged at the same interval as the target 3 1 f. The rod-shaped magnets 43a to 43f are arranged inside the ring-shaped magnets 42a to 42f, and are arranged along the longitudinal direction of the targets 3 1 a to 3 1 f. The rod-shaped magnets 43a to 43f are in a state where ring-shaped magnets 42a to 42f are formed on both sides in the longitudinal direction. Among the magnets of the magnetic field forming means 40a to 40f, the magnets (ring magnets) arranged as the first magnets 42a to 42f, and the magnets (rod magnets) arranged between the magnets 42a to 4 2f are set to the first, and the other The surface area 3 5 a to other components of the magnetic field shape 31a to 42f; 43a to 31a to the side parallel to the ring with 31a to the side. Therefore, the first two magnets on both sides-12- 200538568 〇) 43a to At 43f, the first magnetic poles 42a to 42f and the younger magnets 43a to 43f are located at both ends in the thickness direction, that is, at the front side and the back side. When facing the target 3 1 a to 3 1 f When the side surface is a surface, plate-shaped yokes 4 1 a to 4 1 f are closely adhered to the back sides of the first magnets 4 2 a to 4 2 f and the second magnets 4 3 a to 4 3 f. Therefore, the magnetic force lines generated between the magnetic poles on the back side of the first magnets 42 & to 42f and the second magnets 43a to 43f > pass through the inside of the yokes 4 1 a to # 4 1 f. The planar shapes of the yokes 4 1 a to 4 1 f are equal to the outer periphery of the ring shape of the first magnets 42 a to 42 f. The first magnets 42 a to 42 f are arranged so as not to protrude from the edges of the yokes 4 1 a to 4 1 f. . As described above, the shapes of the first magnets 42a to 42f are substantially equal to those of the targets 31a to 3If, and therefore, the planar shapes of the magnetic field forming means 40a to 40f are also substantially equal to those of the targets 31a to 3f. Here, the respective magnetic field forming means 40a to 40f are arranged at the front and back positions of the corresponding k 1 targets 3 1 a to 3 1 f, so the respective magnetic field forming means Φ 403 to 40f will not pass from the target 31a. The outer perimeters of 31 to 31f protrude, and the respective magnetic field forming means 40a to 40f are not arranged to straddle the two targets 31a to 31. When the magnetism on the surface side of the first magnet 42a to 42f is N-pole, the second magnet 43a The magnetic properties of the magnetic poles on the surface side to 43f are s poles. When the magnetic properties of the magnetic poles on the surface side of the first magnets 42a to 42f are S poles, the magnetic properties of the magnetic poles on the surface side of the second magnets 43a to 43f are N poles. Therefore, a magnetic field line passing through the electrodes 35a to 35f is formed between the surfaces of the first magnets 42a to 42f and the surfaces of the second magnets 43a to 43f. -13- 200538568 (10) The positions inside the electrodes 3 5 a to 3 5 f on the second magnets 4 3 a to 4 3 f are respectively arranged with a material of permeabi 1 ity (in this system Magnetic bodies 36a to 36f with a purity of 99.8% pure iron), and the magnetic lines of force passing through the electrodes 35a to 3f are attracted to the targets 3a to 3f by the magnetic bodies 36a to 36f, And pass through the surfaces of the targets 3 1 a to 3 1 f.

各濺射部30a至3 Of的第一磁鐵42a至42f的相同磁 性的磁極係位在相同面側,因此,第一磁鐵42a至42f的 靶材3 1 a至3 1 f側的極性均爲N極或均爲S極之任一者。 如上所述,第二磁鐵43a至43f之與第一磁鐵42a至 42f相同面側之磁極的磁性係與第一磁鐵42a至42f呈相 反,所以第一磁鐵42a至42f.之靶材31a至3 If側的極性 均爲N極時,第二磁鐵43a至43f之靶材31a至3 I f側的 極性均成S極,當第一磁鐵42a至42f之靶材31a至3 If 側的極性均爲S極時,第二磁鐵4 3 a至4 3 f之靶材3 1 a至 3 1 f側的極性均成N極。 因此,在相同濺射部30a至3 Of之第一磁鐵42a至 42f、第二磁鐵43a至43f之間形成有磁力線,但是在不 同濺射部30a至30f之相鄰第一磁鐵42a至42f之間並未 形成有磁力線。 濺射源3係具有輔助磁場形成手段15a、15b。輔助 磁場形成手段15a、15b係由與第一磁鐵42a至42f長度 大致相等的長度的細長棒狀磁鐵所構成,且沿著第一磁鐵 42a至42f之長邊方向配置在排列有第一磁鐵42a至42 f -14- 200538568 (11) 之區域外側。 輔助磁場形成手段1 5 a、1 5 b係位在與第一磁 至42f、第二磁鐵43a至43f相同的高度。第1圖 符號42a與42f係表示在第一磁鐵42a至42f中, 列前頭與結尾的第一磁鐵。位在行列前頭與結尾的 鐵4 2a、42f之2個長邊方向的側面中,將面向外 側面設爲端部面,而非將朝向行列之中心方向的側 端部面時,該端部面係與輔助磁場形成手段1 5 a、 長邊方向的側面密接或間離。The same magnetic poles of the first magnets 42a to 42f of each of the sputtering sections 30a to 3Of are located on the same surface side. Therefore, the polarities of the target 3 1a to 3 1 f sides of the first magnets 42a to 42f are all The N pole may be either the S pole. As described above, the magnetic systems of the magnetic poles on the same surface side of the second magnets 43a to 43f as the first magnets 42a to 42f are opposite to those of the first magnets 42a to 42f, so the targets 31a to 3 of the first magnets 42a to 42f. When the polarity on the If side is all N, the polarities on the targets 31a to 3f of the second magnets 43a to 43f are all S poles, and when the polarity on the If 31a to 3f of the first magnets 42a to 42f are all on the If side, In the case of the S pole, the polarities of the targets 3 1 a to 3 1 f of the second magnets 4 3 a to 4 3 f are all N poles. Therefore, magnetic lines of force are formed between the first magnets 42a to 42f and the second magnets 43a to 43f in the same sputtering portions 30a to 3Of, but between adjacent first magnets 42a to 42f in different sputtering portions 30a to 30f. There were no magnetic lines of force formed between them. The sputtering source 3 includes auxiliary magnetic field forming means 15a and 15b. The auxiliary magnetic field forming means 15a and 15b are constituted by an elongated rod-shaped magnet having a length approximately equal to the length of the first magnets 42a to 42f, and the first magnets 42a are arranged along the longitudinal direction of the first magnets 42a to 42f. Up to 42 f -14- 200538568 (11) outside the area. The auxiliary magnetic field forming means 15a, 15b are located at the same height as the first magnets 42f and the second magnets 43a to 43f. In Fig. 1, symbols 42a and 42f indicate the first magnets at the head and the end of the first magnets 42a to 42f. Of the two long sides of the iron 4 2a, 42f located at the front and end of the rank, the end face is the end face instead of the side end face facing the center of the rank. The surface system is in close contact with or separated from the auxiliary magnetic field forming means 15a.

第3圖係表示第一磁鐵42a至42f、第二磁鐵 4 3 f與輔助磁場形成手段1 5 a、1 5 b之磁極關係之一 輔助磁場形成手段1 5 a、1 5 b的磁極係位在厚度方 端,亦即位在表面側與背面側,當將朝向與第一磁 至42f、第二磁鐵43a至43f之表面相同側的面設 時,輔助磁場形成手段15a、15b的背面係密接 16a、16b,因此,從輔助磁場形成手段15a、15b 側的磁極發生的磁力線係通過磁軛1 6a、1 6b的內音C 輔助磁場形成手段1 5 a、1 5 b之表面側之磁極 係與第一磁鐵42a至42f之表面側之磁極的磁性相 此,第一磁鐵42a至42f之表面側之磁極的磁性| 時,輔助磁場形成手段1 5 a、1 5 b之表面側之磁極 爲N極,當第一磁鐵42a至42f之表面側之磁極的 S極時,輔助磁場形成手段1 5 a、1 5 b之表面側之 磁性則爲S極。 鐵42a 的元件 位在行 第一磁 方向的 面設爲 15b之 43a至 例圖。 向的兩 鐵42a 爲表面 於磁軛 之背面 > ° 的磁性 同。因 i n極 的磁性 磁性爲 磁極的 -15- 200538568 (12) 如上所述,輔助磁場形成手段1 5a、〗5b係以沿著位 在最外側的第一磁鐵4 2 a、4 2 f的方式予以配置’所以輔 助磁場形成手段1 5 a、1 5 b與位於最外側的第一磁鐵 42a、42f作爲1個磁鐵而發揮作用,且在該磁鐡表面與相 鄰之第二磁鐵4 3 a、4 3 f表面之間,會發生通過位於最外 側之靶材3 1 a、3 1 f的磁力線。FIG. 3 shows the magnetic pole positions of the auxiliary magnetic field forming means 1 5 a and 1 5 b, which is one of the magnetic pole relationships between the first magnets 42 a to 42 f, the second magnet 4 3 f, and the auxiliary magnetic field forming means 1 5 a, 1 5 b. At the thickness end, that is, on the front side and the back side, when the surfaces facing the same side as the surfaces of the first magnet 42f and the second magnet 43a to 43f are provided, the back surfaces of the auxiliary magnetic field forming means 15a and 15b are closely contacted. 16a, 16b. Therefore, the magnetic field lines generated from the magnetic poles on the auxiliary magnetic field forming means 15a and 15b pass through the internal sounds of the yokes 16a and 16b. The magnetic pole system on the surface side of the auxiliary magnetic field forming means 15a and 15b. In contrast to the magnetic properties of the magnetic poles on the surface side of the first magnets 42a to 42f, when the magnetic properties of the magnetic poles on the surface side of the first magnets 42a to 42f |, the magnetic poles on the surface side of the auxiliary magnetic field forming means 1 5 a, 1 5 b When the N pole is the S pole of the magnetic pole on the surface side of the first magnets 42a to 42f, the magnetic force on the surface side of the auxiliary magnetic field forming means 15a, 15b is the S pole. The element of iron 42a is located on the surface in the first magnetic direction of the row and is set to 43a to 15b. The two irons 42a facing each other have the same magnetic properties as the surface on the back of the yoke. Because the magnetic polarity of the in-pole is -15-200538568 (12) As mentioned above, the auxiliary magnetic field forming means 15a and 5b are along the first magnets 4 2a and 4 2 f located at the outermost side. It is arranged so that the auxiliary magnetic field forming means 1 5 a and 1 5 b and the outermost first magnets 42 a and 42 f function as one magnet, and the surface of the magnetic field and the adjacent second magnet 4 3 a Between 3 and 4 3 f surfaces, magnetic lines of force passing through the outermost targets 3 1 a and 3 1 f will occur.

在此,位在行列前頭與結尾之靶材3 1 a、3 1 f之2個 長邊方向的側面中,並非是朝向行列之中心方向的側面, 而是在面向外方向的側面的正下方,設有第一磁鐵42a、 42f的端部面。 因此,輔助磁場形成手段1 5 a、1 5 b係配置在比位在 最外側之耙材3 1 a、3 1 f的正背面位置還外側的位置,通 過位在最外側之靶材3 1 a、3 1 f的表面的磁力線的磁通強 度,即便位在該靶材 3 1 a、3 1 f的端部位置,亦不會變 弱。 第6圖係並列配置5個濺射部3 0a至3 0e,當接近位 在最外側之第一磁鐵1 5 a、1 5 e而配置輔助磁場形成手段 1 5 a、1 5 b時,將測定靶材3 1 a至3 1 e表面之磁通密度後 的結果,與磁場形成手段40a至40e及輔助磁場形成手段 15a、15b的位置一起表示的圖。此外,第6圖與後述之 第7圖的元件符號係分別表示爲:Bv係相對於靶材3 1 a 至3 1 e表面爲垂直方向的磁通密度,Bll係相對於靶材3 1 a 至3 I e表面爲平行方向的磁通密度,橫軸係將5個靶材 3 1 a至3 1 e之行列中央位置設爲〇時之距離中央的距離, -16- 200538568 (13) 縱軸係磁通密度(G :高斯(G au s s ))。 如第6圖所示,磁通密度之平行方向的分布爲梯形, 而且垂直方向的分布係顯示以0爲交差的點有2點以上 (在此爲3點)的形狀。藉由形成上述磁場形狀的磁力 線,即使不搖動磁鐵,在後述之濺射製程中·,各靶材3 1 a 至3 1 e的幾乎整面會受到濺射,可推測出可實現幾乎沒有 I 非侵蝕部分的狀態。 # 再者,藉由配置輔助磁場形成手段15a、Mb,即使 在位在最外側之靶材3 1 a、3 1 f的寬度方向的端部,亦可 維持與中央部分相同程度的磁場強度。 相對於此,第7圖係未配置輔助磁場形成手段1 5a、 1 5 b時,將測定各耙材3 1 a至3 1 e表面之磁通密度的結 果,與磁場形成手段40a至40e的位置關係一同表示的 圖。此時的磁通密度之平行方向的分布爲梯形,而且垂直 I 方向的分布係顯示以〇爲交差的點有2點以上的形狀,但 • 是由於磁場形成手段40a至40e彼此相鄰接,所以基於磁 場形成手段40a至40e彼此的磁場干擾,在靶材31a至 3 1 e之行列兩端部會使磁場強度失去平衡,磁通密度會比 濺射源3的中央部分還弱。 接著,就使用該成膜裝置1而在基板表面形成薄膜的 製程加以說明。成膜裝置1係具有分別與真空槽2相連接 的真空排氣系統1 2與氣體供應系統1 3,藉由真空排氣系 統1 2對真空槽2內部進行真空排氣時,在靶材3 ] a至3 1 f 之相互對向的側面之間亦進行真空排氣,而在該區域形成 -17- 200538568 (14) 真空環境氣體。 第1圖的符號s係表示靶材3 1 a至3 1 f之相互對向的 側面彼此間之距離,在本發明之成膜裝置]中,係在相鄰 的靶材3 1 a至3 1 f間並未配置電極或屏蔽等固體或如冷卻 水的液體,靶材3 1 a至3 1 f之長邊方向的側面係僅透過真 空槽2內部的環境氣體而直接相對向。因此,形成在靶材 3 1 a至3 1 f之相互對向之側面之間的真空環境氣體之側面 彼此間的距離s方向的長度係與側面彼此間之距離s的長 度相同。 接著,一面持續進行真空排氣,一面由氣體供應系統 1 3 —起供應濺射氣體與反應性氣體,而在真空槽2內部 形成預定壓力之成膜環境氣體.。預先在基板保持具4保持 基板5,且在將基板5與真空槽2置於接地電位的狀態 下 17 面維持成膜環境氣體 面起動交流電源17a至 如上所述,當由交流電源17a至17c施加 1kHz以 上、100kHz以下的交流電壓時,相鄰的2個靶材31a至 3 1 f中的一個置於相對於接地電位的正電位,另一個置於 相對於接地電位的負電位,因此,置於正電位的耙材3 1 a 至3 1 f係作爲陽極而發揮作用,置於負電位的靶材3〗a至 3 1 f的濺射面受到濺射,而釋放出濺射粒子。 革巴材3 1 a至3 1 f的電位係按照交流電壓的頻率,由正 電位切換到負電位,或由負電位切換到正電位,因此靶材 3 1 a至3 1 f係交替受到濺射,結果使得所有靶材3 1 a至 - 18- 200538568 (15) 3 1 f受到濺射。 當將基板5之形成膜的面設爲成膜面時,基板5之成 膜面係配置成與各靶材3 1 a至3 1 f之濺射面相對向,因此 由濺射面釋放出的濺射粒子會到達基板5的表面,且在基 板5的表面與反應性氣體起反應,而在基板5的表面成長 由靶材材料與反應性氣體進行反應的反應物構成的膜。 如上所述,在相鄰之靶材3 1 a至3 1 f之間並未配置任 Φ 何構件,靶材3 1 a至3 1 f之相互對向的側面彼此間之距離 s變得很小,爲1 mm以上、1 0mm以下,由於該距離s較 小之故,所以未釋放出濺射粒子之面積比率會變小。因 此,濺射粒子均勻地到達基板5表面,結果使得形成在基 板5表面的膜的膜厚分布變得均勻.。 此外,該成膜裝置1係具有作爲防著板之屏蔽丨1, > 屏蔽1 1係配置成:圍繞排列濺射部3 0a至3 〇f之區域的 周圍以及輔助場形成手段1 5 a、1 5 b,雜射面以外的部 ® 分係形成不會由屏蔽1 1露出。因此,電極35a至35f或 磁場形成手段4〇a至40f係藉由該屏蔽n而與機射粒子 形成遮蔽,因此不會附著濺射粒子。 (實施例) <實施例> 、長度 式進行 1 000 人 使用上述成膜裝置1 ’將寬度Hoomm 125 0mm、厚度0.7mm的玻璃基板5以不加熱的方 3〇秒鐘的濺射’而在基板5表面形成膜厚 -19-Here, the sides of the two long sides of the targets 3 1 a and 3 1 f at the front and end of the rank are not the side facing the center of the rank, but directly below the side facing outward. The end faces of the first magnets 42a and 42f are provided. Therefore, the auxiliary magnetic field forming means 1 5 a and 1 5 b are arranged on the outer side than the front and rear positions of the outermost rakes 3 1 a and 3 1 f, and pass through the outermost target 3 1 The magnetic fluxes of the magnetic lines of force on the surfaces of a and 3 1 f will not weaken even if they are located at the ends of the targets 3 1 a and 3 1 f. Fig. 6 shows that five sputter sections 30a to 3e are arranged in parallel. When the first magnets 15a and 15e located near the outermost side are arranged and the auxiliary magnetic field forming means 1a and 15b are arranged, The results of measuring the magnetic flux densities on the surfaces of the targets 3 1 a to 3 1 e are shown together with the positions of the magnetic field forming means 40 a to 40 e and the auxiliary magnetic field forming means 15 a and 15 b. In addition, the component symbols in FIG. 6 and FIG. 7 described below are respectively expressed as: Bv is a magnetic flux density perpendicular to the surface of the target 3 1 a to 3 1 e, and Bll is relative to the target 3 1 a The surface to 3 I e surface is the magnetic flux density in the parallel direction. The horizontal axis is the distance from the center when the center position of the 5 targets 3 1 a to 3 1 e is set to 0. -16-200538568 (13) Shaft magnetic flux density (G: Gauss (G au ss)). As shown in Fig. 6, the distribution of the magnetic flux density in the parallel direction is trapezoidal, and the distribution in the vertical direction shows a shape with two or more points crossing at 0 (three points here). By forming the magnetic field lines of the aforementioned magnetic field shape, even if the magnet is not shaken, in the sputtering process described later, almost the entire surface of each target 3 1 a to 3 1 e is sputtered, and it is estimated that almost no I Status of non-eroded parts. # Furthermore, by arranging the auxiliary magnetic field forming means 15a and Mb, the magnetic field strength at the same level as the central portion can be maintained even at the widthwise ends of the outermost targets 3 1 a and 3 1 f. In contrast, in Fig. 7, when the auxiliary magnetic field forming means 15a and 15b are not provided, the results of measuring the magnetic flux density on the surface of each of the rake materials 3 1a to 3 1e are compared with those of the magnetic field forming means 40a to 40e. Figure showing positional relationship. The parallel distribution of the magnetic flux density at this time is trapezoidal, and the distribution in the vertical I direction shows that the points crossing at 0 have a shape of more than 2 points, but • the magnetic field forming means 40a to 40e are adjacent to each other, Therefore, based on the magnetic field interference of the magnetic field forming means 40a to 40e, the magnetic field intensity is unbalanced at the two ends of the rows of the targets 31a to 3e, and the magnetic flux density is weaker than the central part of the sputtering source 3. Next, a process for forming a thin film on a substrate surface using the film forming apparatus 1 will be described. The film forming apparatus 1 has a vacuum exhaust system 12 and a gas supply system 13 connected to the vacuum tank 2 respectively. When the inside of the vacuum tank 2 is evacuated by the vacuum exhaust system 12, the target 3 ] A to 3 1 f are also evacuated between the opposite sides, and -17- 200538568 (14) vacuum ambient gas is formed in this area. The symbol s in FIG. 1 indicates the distance between the opposite sides of the targets 3 1 a to 3 1 f. In the film forming apparatus of the present invention], the targets 3 1 a to 3 are adjacent to each other. Between 1 f, there is no solid such as electrode or shield, or liquid such as cooling water, and the side surfaces in the longitudinal direction of the targets 3 1 a to 3 1 f are directly opposed to each other only through the ambient gas in the vacuum tank 2. Therefore, the length in the direction of the distance s between the sides of the vacuum environment gas formed between the opposing sides of the targets 3 1 a to 3 1 f is the same as the length of the distance s between the sides. Next, while the vacuum evacuation is continuously performed, the sputtering gas and the reactive gas are supplied from the gas supply system 1 to form a film-forming ambient gas at a predetermined pressure inside the vacuum tank 2. The substrate 5 is held in the substrate holder 4 in advance, and the substrate 5 and the vacuum chamber 2 are placed at the ground potential. The film is maintained on the 17 side. The ambient gas is turned on. The AC power source 17a is started as described above. When the AC power source 17a to 17c is used, When an AC voltage of 1 kHz to 100 kHz is applied, one of the two adjacent targets 31a to 3 1 f is placed at a positive potential with respect to the ground potential, and the other is placed at a negative potential with respect to the ground potential. The rake materials 3 1 a to 3 1 f placed at a positive potential function as anodes, and the sputtering surfaces of the targets 3 a to 3 1 f placed at a negative potential are sputtered to release sputtered particles. The potential of the leather materials 3 1 a to 3 1 f is switched from a positive potential to a negative potential, or from a negative potential to a positive potential according to the frequency of the AC voltage. Therefore, the targets 3 1 a to 3 1 f are alternately splashed. As a result, all targets 3 1 a to -18 200538568 (15) 3 1 f were subjected to sputtering. When the film-forming surface of the substrate 5 is set as the film-forming surface, the film-forming surface of the substrate 5 is arranged to face the sputtering surfaces of the respective targets 3 1 a to 3 1 f, and therefore is released from the sputtering surface. The sputtered particles reach the surface of the substrate 5, and react with the reactive gas on the surface of the substrate 5, and a film made of a reactant that reacts with the target material and the reactive gas grows on the surface of the substrate 5. As described above, no member is arranged between the adjacent targets 3 1 a to 3 1 f, and the distance s between the opposite sides of the targets 3 1 a to 3 1 f becomes very large. It is smaller than 1 mm and not more than 10 mm, and since the distance s is small, the area ratio of sputtered particles that are not released becomes small. Therefore, the sputtered particles reach the surface of the substrate 5 uniformly, and as a result, the film thickness distribution of the film formed on the surface of the substrate 5 becomes uniform. In addition, the film forming apparatus 1 has a shield serving as an anti-plate, and the shield 1 1 is configured to surround the area where the sputtering portions 30a to 30f are arranged and the auxiliary field forming means 15a. , 1 5 b, parts other than the diffusive surface are formed so that they are not exposed by the shield 1 1. Therefore, since the electrodes 35a to 35f or the magnetic field forming means 40a to 40f are shielded from the machine-projected particles by the shield n, the sputtered particles are not attached. (Examples) < Examples > The length-formed method was performed by 1,000 people using the film-forming apparatus 1 'sputtering a glass substrate 5 having a width of Hoomm 125 0 mm and a thickness of 0.7 mm in 30 seconds without heating' And a film thickness of -19- is formed on the surface of the substrate 5

200538568 (16) (1 OOnn])的 ITO ( Indium Tin Oxide,銦錫氧化物)膜。 在此係使用6塊由In2〇3-l〇W%Sn02 ( ITO )構成之 寬度200mm、長度1 7 0 0、厚度的靶材31a至31f, 將各靶材3 1 a至3 1 f配置成與基板5的寬度方向平行,且 距離s爲2mm。磁場形成手段40a至4 0f的寬度係與靶材 3 1 a至3 1 f相同,爲2 0 0 m m。由氣體供應系統1 3供應 2 0 0 s c c m之灑射氣體的A r氣’同時亦供應反應性热B豆 (Η 2 Ο、Ο 2 ),爲了控制最適流量,將各反應性氣體的流 量在Osccm以上、5sccm以下之間變化,而形成〇.7Pa的 成膜環境氣體。交流電壓的施加係將輸出從0kw慢慢上 升,最後投入到20kw爲止。交流電壓的頻率爲50kHz。 將成膜後的ITO膜的膜厚以35點進行測定。其測定 結果表示於第5圖。 如第5圖所示,基板5面內的膜厚偏差較小,膜厚分 布係以3 5點測定,可得± 8 %之良好的値。由此可知,在 濺射中,電漿的偏差較小。此外,在進行濺射時,並未見 到異常放電,放電亦呈穩定狀態,混入於成膜後的膜中的 微粒亦幾乎無法看到。 此外,不使用〇2氣體作爲反應性氣體,而僅使用 H2〇氣體,除了使H2〇氣體流量由Osccm變化到5sccm 之外,以與上述實施例相同的條件進行成膜,形成ITO 膜,且分別測定在成膜瞬後之ITO膜的片電阻(Sheet Resistance ) ( Ω / □)以及在成膜後進行加熱處理(退 火化處理)者的片電阻(Ω / □),在成膜瞬後,即使在 - 20-200538568 (16) (100 nn)) of ITO (Indium Tin Oxide) film. Here, six targets 31a to 31f with a width of 200 mm, a length of 1700, and a thickness of In2〇3-10W% Sn02 (ITO) are used, and the targets 3 1 a to 3 1 f are arranged. It is parallel to the width direction of the substrate 5, and the distance s is 2 mm. The widths of the magnetic field forming means 40a to 40f are the same as those of the targets 3a to 31f, and are 200 m. The Ar supply gas of 2 0 0 sccm of the spray gas is supplied from the gas supply system 13 and the reactive hot B beans (Η 2 〇, Ο 2) are also supplied. In order to control the optimal flow rate, the flow rate of each reactive gas is adjusted between It changes between above Osccm and below 5 sccm to form a film-forming ambient gas of 0.7 Pa. The AC voltage is applied to gradually increase the output from 0kw, and finally to 20kw. The frequency of the AC voltage is 50 kHz. The film thickness of the ITO film after film formation was measured at 35 points. The measurement results are shown in Fig. 5. As shown in Fig. 5, the variation of the film thickness in the five planes of the substrate is small. The film thickness distribution is measured at 35 points, and a good 値 of 8% can be obtained. From this, it can be seen that the variation of the plasma is small during sputtering. In addition, during sputtering, no abnormal discharge was observed, and the discharge was stable. The particles mixed in the film after film formation were hardly visible. In addition, instead of using O 2 gas as the reactive gas, only H 2 O gas was used, except that the H 2 O gas flow rate was changed from Osccm to 5 sccm, and film formation was performed under the same conditions as in the above embodiment to form an ITO film, and The sheet resistance (Ω / □) of the ITO film after the film formation instant and the sheet resistance (Ω / □) of the heat treatment (annealing process) after the film formation were measured separately. After the film formation instant, , Even at-20-

200538568 (17) 改變氣體流量的情形下,片電阻並不會改變,且顯示 的値。相較於成膜瞬後的情形,在經退火化的情形下 電阻値較低,尤其是Η 2 〇氣體流量爲2 s c c m時,其 阻最低。 再者,使用 H20氣體及02氣體雙方作爲反應 體,將Η 2 〇氣體流量固定爲2 s c c m,且使〇 2氣體流 0 s c c m到2.0 s c c m之間變化,來進行I Τ Ο膜的成膜, 定成膜瞬後及進行退火化處理後之片電阻(Ω /□) 較於成膜瞬後的情形,在經退火化的情形下的片電阻 低’尤其是〇2氣體流星爲l.Osccm時’其片電阻最 因此可知反應性氣體的最適流量爲:Η 2 0氣體爲2 s c 〇 2氣體爲1 S c c m。 再者,在求出當反應性氣體流量爲最適流量時之 膜的片電阻分布時,片電阻的最大値爲26.8Ω / □, 値爲23.4Ω/ □,平均値爲25.1Ω/ □,片電阻分布 6.7%。由此可知,若使用本發明之成膜裝置1,可得 阻分布良好的ITO膜,其片電阻分布並未形成反映出 之形狀或配置的分布。 再者,以本發明之成膜裝置1進行長時間成膜時 電穩定,且未見到異常放電。在放電後,經確認ITO 31a至31f表面之後,在靶材31a至31f表面並未見 侵蝕區域。 <比較例> 較高 的片 片電 性氣 量在 且測 ,相 値較 低。 cm、 ITO 最小 爲土 片電 靶材 ,放 靶材 到非 -21 - 200538568 (18) 作爲成膜裝置,配置寬度(1 3 0 m m寬)小於粑材3 1 a 至3 1 f的棒狀磁鐵,來替代上述成膜裝置1之磁場形成手 段40a至40f ’且朝靶材之寬度方向搖動8〇nim,且由外 部進行控制,俾使靶材表面磁場隨時間發生變化。棒狀磁 鐵的搖動速度係進行1 0 m m / s e c之等速反轉控制。200538568 (17) In the case of changing the gas flow rate, the sheet resistance does not change, and 値 is displayed. Compared with the case immediately after film formation, the resistance 値 is lower in the case of annealing, especially when the Η 2 gas flow rate is 2 s c c m, and the resistance is the lowest. In addition, using both H20 gas and 02 gas as the reactants, the Η 2 〇 gas flow rate was fixed to 2 sccm, and the 〇 2 gas flow was changed from 0 sccm to 2.0 sccm to perform the ITO film formation. The sheet resistance (Ω / □) after the film formation instant and after the annealing treatment is lower than the case after the film formation instant, and the sheet resistance is lower in the case of annealing, especially the 0 2 gas meteor is l.Osccm At this time, its sheet resistance is the best. It can be seen that the optimal flow rate of the reactive gas is: Η 2 0 gas is 2 sc 〇 2 gas is 1 S ccm. In addition, when the sheet resistance distribution of the film when the reactive gas flow rate is the optimum flow rate is obtained, the maximum sheet resistance 値 is 26.8Ω / □, 値 is 23.4Ω / □, and the average 値 is 25.1Ω / □. Resistance distribution 6.7%. From this, it can be seen that if the film-forming apparatus 1 of the present invention is used, an ITO film having a good resistance distribution can be obtained, and the sheet resistance distribution does not form a reflected shape or arrangement. Furthermore, the film-forming apparatus 1 of the present invention is electrically stable during long-term film formation, and no abnormal discharge is observed. After the discharge, after confirming the surfaces of the ITO 31a to 31f, no erosion area was seen on the surfaces of the targets 31a to 31f. < Comparative example > The higher the chip electric capacity is, the lower the phase contrast is. cm, ITO minimum soil chip electric target, put the target to a non--21-200538568 (18) as a film-forming device, the width of the configuration (130 mm wide) is smaller than the rod 3 1 a to 3 1 f A magnet is used in place of the magnetic field forming means 40a to 40f 'of the film forming apparatus 1 described above, and is shaken 80 nm toward the width of the target, and is controlled externally so that the magnetic field on the target surface changes with time. The rocking speed of the rod-shaped magnet is controlled at a constant speed of 10 m m / s e c.

靶材3 1 a至3 1 f係使用與上述實施例相同者,以隔出 相同間隔的方式配置。成膜環境氣體係由氣體供應系統 13供應200sccm之Ar氣體,而形成〇.7Pa的壓力。以頻 率5 0 k Η z將相鄰之靶材3 1 a至3 1 f的電位進行正負切換, 電力由Okw慢慢上升之後,當投入1 〇kw之電力時,在靶 材上可以目測確認到激烈的異常放電,而變得無法投入更 多的電力。在進行放電測試之後,當確認真空槽內後,於 屏蔽1 1中確認出異常放電痕。由上可知,若使用本發明 之成膜裝置1,在濺射時不會發生異常放電,而且在靶材 中亦不會形成非侵蝕區域。 以上係就對於相鄰之靶材3 1 a至3 1 f由相同的交流電 源1 7a至1 7c施加交流電壓的情形加以說明,惟本發明並 非限定於此。如第4圖所示,亦可對於未相鄰接之不同的 2個靶材3 1 a至3 1 f由相同的交流電源1 7a至1 7c施加交 流電壓。此時,以交替置於不同於相鄰之靶材3 1 a至3 1 f 之極性的電位的方式,來施加電壓爲宜。 曰曰 以上係就由_ ITO構成的透明導電膜進行說明,惟本發 明之成膜裝置的成膜目的並非特別限定’亦可形成金屬薄 膜、透明導電膜、介電體膜等各種膜,來用於製造液 -22 - 200538568 (19) PDP ( Plasma display panel,電漿顯示面板)或 FED (Field Emission D i s p 1 a y,場發射顯示器)或 EL (E1 e c 11· o L u m i n e s c e n c e,電激發光)等平面顯示器。The targets 3 1 a to 3 1 f are arranged at the same intervals using the same ones as in the above-mentioned embodiment. The film-forming ambient gas system was supplied with 200 sccm of Ar gas by the gas supply system 13 to form a pressure of 0.7 Pa. The potential of the adjacent targets 3 1 a to 3 1 f is switched between positive and negative at a frequency of 50 k Η z. After the power is gradually increased from Okw, when 10 kw of power is input, it can be confirmed visually on the target. To intense abnormal discharge, it becomes impossible to put in more power. After performing the discharge test, after confirming the inside of the vacuum chamber, abnormal discharge marks were confirmed in the shield 11. As can be seen from the above, if the film-forming device 1 of the present invention is used, abnormal discharge does not occur during sputtering, and a non-eroded region is not formed in the target. The above description has been made of the case where the adjacent target materials 3 1 a to 3 1 f are applied with the AC voltage by the same AC power sources 17 a to 17 c, but the present invention is not limited thereto. As shown in Fig. 4, it is also possible to apply an AC voltage to two different targets 3 1 a to 3 1 f that are not adjacent to each other from the same AC power source 17 a to 17 c. At this time, it is preferable to apply a voltage in such a manner that a potential different from that of the adjacent targets 3 1 a to 3 1 f is applied. The above is a description of the transparent conductive film made of ITO, but the film-forming purpose of the film-forming device of the present invention is not particularly limited. Various films such as metal thin films, transparent conductive films, and dielectric films can also be formed. Used to manufacture liquid-22-200538568 (19) PDP (Plasma display panel) or FED (Field Emission D isp 1 ay) or EL (E1 ec 11. · Lumininescence) ) And so on flat display.

本發明中所使用的基板5並非特別限定者,亦可使用 玻璃基板、附有樹脂膜之基板、或樹脂基板等各種基板。 根據本發明,藉由使用複數個靶材3 1 a至3 1 f,來使成膜 面積變大,因此亦可在平面形狀之面積爲1 m2以上的大型 基板表面形成薄膜。 當將磁場形成手段40a至4 Of配置在與靶材31a至 3 If相同的真空槽2內部時,最好在磁鐵42a至42 f、43 a 至4 3 f以及磁軛4 1 a至4 1 f的表面施加不會對經濺射成膜 後的膜質造成影響的材質或表面處理以及其與輾材之接著 方法。再者,由於處於與放電空間相同的環境氣體中,因 此以使磁場形成手段4 0 a至4 0 f之S極、N極間的空間不 會產生電漿的方式,以爲非磁性體且施加對經濺射成膜後 的膜質不會造成影響之表面處理的材料,充滿S極、N極 間的空間爲宜。 以上係就磁性體36a至36f配置在電極35a至35f之 內部的情形加以說明,但本發明並非限定於此,只要形成 有如上所述之第6圖所示之磁場形狀的磁力線,即使不配 置例如磁性體36a至36f亦可,此外,當配置磁性體36a 至3 6f時’其位置並非特別有所限定,而亦可將例如磁性 體36a至36f配置在與第—磁鐵42a至42f、第二磁鐵 43a至43f相同的磁軛41a至4]f之上。 -23-The substrate 5 used in the present invention is not particularly limited, and various substrates such as a glass substrate, a substrate with a resin film, or a resin substrate may be used. According to the present invention, a plurality of targets 3 1 a to 3 1 f are used to increase the film formation area, so that a thin film can be formed on the surface of a large substrate having a planar area of 1 m 2 or more. When the magnetic field forming means 40a to 4 Of are disposed inside the same vacuum chamber 2 as the targets 31a to 3 If, it is preferable to place the magnets 42a to 42f, 43a to 43f, and the yoke 41a to 41. The surface of f is applied with a material or surface treatment that does not affect the film quality after being sputtered into a film, and a method for bonding it to a rolled material. Furthermore, since it is in the same ambient gas as the discharge space, a plasma is not generated in the space between the S and N poles of the magnetic field forming means 40 a to 40 f, so that it is non-magnetic and is applied. It is advisable to fill the space between the S and N poles for the surface-treated materials that do not affect the film quality after sputtering. The above is a description of the case where the magnetic bodies 36a to 36f are arranged inside the electrodes 35a to 35f. However, the present invention is not limited to this, as long as the magnetic field lines of the magnetic field shape shown in FIG. For example, the magnetic bodies 36a to 36f may be used. In addition, when the magnetic bodies 36a to 36f are arranged, their positions are not particularly limited, and for example, the magnetic bodies 36a to 36f may be arranged in the first and second magnets 42a to 42f. The two magnets 43a to 43f are above the same yokes 41a to 4] f. -twenty three-

200538568 (20) 此外,只要形成有如上所述之第6圖坷 的磁力線,第一磁鐵4 2 a至4 2 f、第二磁鐵 形狀、配置、數量亦非特別有所限定。 各祀材3 1 a至3 1 f的長度係大於進行成 度,其一例爲1 5 00mm以上、2000mm以下 材31a至3 1f之寬度之一例係l〇〇mm以. 下。 靶材之台數之一例爲,以靶材台數X靶 台數X靶材間距離表示之陰極外形W爲基 台數,其一例爲成爲1 2 0 0 m m s W $ 1 9 0 0 m m 相鄰靶材3 1 a至3 1 f之相互對向的側面 一例爲1mm以上、1 〇mm以下 '。由靶材3 j a 面到基板5的成膜面爲止的距離之一例爲 3 0 0 m m以下。 耙材3 1 a至3 1 f之濺射面係以配置於 宜。耙材3 1 a至3 ! f之厚度雖未特別有所限 爲5mm以上、30mm以下。 若在電極35a至35f安裝冷卻手段,則 材3 1 a至3 1 f,〜面進行濺射。安裝靶材3 ! 極3 5 a至3 5 f的厚度並未特別有所限定,$ 以上、3 0 m m以下。 用以將靶材31a至3 If以及電極35a至 成手段40a至4〇f作電性絕緣之絕緣板33a 的一例爲2 m m以上、丨〇 ni m以下。 •示之磁場形狀 43a至43f之 膜之基板的長 。此外,各靶 上、4 0 0 m m以 材寬度+靶材 板寬度以上之 的台數。 間的距離s的 至3 1 f的濺射 6 0 m m以上、 相同平面上爲 定,但其一例 可一面冷卻靶 a至3 1 f的電 霉一例爲5 m m 35f與磁場形 至33f之厚度 -24- 200538568 (21) 此外,在真空槽2內部,沿著靶材3 1 a至3 1 f的長邊 方向,配置氣體管,藉由該氣體管,從相鄰之靶材3 1 a至 3 1 f之間使濺射氣體或反應性氣體流通,而對放電空間直 接供應氣體,因此變得難以落入供應限速。此時,若在基 板側面周圍設置排氣口,可使供應至放電空間的氣體快速 排氣。200538568 (20) In addition, the shape, arrangement, and number of the first magnets 4 2 a to 4 2 f and the second magnets are not particularly limited as long as the magnetic field lines of FIG. 6 (i) are formed as described above. The length of each of the materials 3 1 a to 3 1 f is larger than the progress rate, and an example thereof is more than 1500 mm and less than 2000 mm. One example of the width of the materials 31 a to 3 1 f is 100 mm or less. An example of the number of targets is the number of cathodes W, which is expressed by the number of targets X the number of targets X the distance between the targets. The number of bases is an example, and an example is the phase of 1 2 0 0 mms W $ 1 9 0 0 mm Examples of mutually facing side surfaces of the adjacent targets 3 1 a to 3 1 f are 1 mm or more and 10 mm or less'. An example of the distance from the target 3 j a surface to the film-forming surface of the substrate 5 is 300 mm or less. The sputtering surfaces of the rake materials 3 1 a to 3 1 f are preferably arranged. Although the thickness of the rake materials 3 1 a to 3! F is not particularly limited, it is 5 mm or more and 30 mm or less. If a cooling means is attached to the electrodes 35a to 35f, the materials 3 1 a to 3 1 f are sputtered. The thickness of the mounting target 3! Poles 3 5 a to 3 5 f is not particularly limited, but it is more than $ and less than 30 mm. An example of the insulating plate 33a for electrically insulating the targets 31a to 3If and the electrodes 35a to 40f to 40f is 2m m or more and 0nm or less. • The length of the film substrate shown in the magnetic field shapes 43a to 43f. In addition, the number of units on each target, 400 mm m, is greater than the width of the target + the width of the target plate. The distance from s to 3 1 f is more than 60 mm. It is determined on the same plane, but one example can cool the target a to 3 1 f. The one is 5 mm 35 f and the magnetic field is 33 f. -24- 200538568 (21) In addition, inside the vacuum tank 2, a gas tube is arranged along the long side of the target 3 1 a to 3 1 f, and the gas tube is used to pass the adjacent target 3 1 a It allows the sputtering gas or reactive gas to circulate to 3 1 f, and directly supplies the gas to the discharge space, so it becomes difficult to fall into the supply rate limit. At this time, if an exhaust port is provided around the side of the substrate, the gas supplied to the discharge space can be quickly exhausted.

對靶材3 1 a至3 1 f進行電力供應之一例爲,相對於與 1個交流電源1 7a至1 7c相連接之2個靶材3 1 a至3 1 f, 其輸出密度P爲1W/ cm2以上、10W/ cm2以下。此外, 當使用金屬靶材3 1 a至3 1 f時,輸出密度P的一例爲5 w / cm2 以上、40W/ cm2 以下。 此外,對靶材3 1 a至3 1 f進行電力供應之一例爲,爲 了調整基板上之膜厚分布,在複數排列之靶材3 1 a至3 1 f 之中,對於位於最外側之靶材3 1 a、3 1 f之供應係以對於 位於中央位置之靶材3 1 c、3 1 d的供應量的1 〇 〇 %以上、 1 3 0 %以下的方式供應。 此外,在進行濺射時,施加至靶材3 1 a至3 1 f的電壓 之一例爲,相對於接地電位,爲-3 00 0V以上之交流電 壓。 以上係以1個細長磁鐵構成1個輔助磁場形成手段 1 5 a、1 5b的情形加以說明,但本發明並非限定於此,亦 可以複數個磁鐵構成1個輔助磁場形成手段,或是將各磁 鐵沿著靶材的長邊方向,配置在配置有磁場形成手段之區 域的外側。此外,輔助磁場形成手段1 5 a、1 5 b與相鄰之 -25-An example of power supply to the targets 3 1 a to 3 1 f is an output density P of 1 W with respect to two targets 3 1 a to 3 1 f connected to an AC power source 17a to 17c. / cm2 or more, 10W / cm2 or less. When the metal targets 3 1 a to 3 1 f are used, an example of the output density P is 5 w / cm 2 or more and 40 W / cm 2 or less. In addition, as an example of supplying power to the targets 3 1 a to 3 1 f, in order to adjust the film thickness distribution on the substrate, among the targets 3 1 a to 3 1 f arranged in a plurality, for the target located at the outermost side The materials 3 1 a and 3 1 f are supplied in a manner of 100% or more and 130% or less of the supply amount to the targets 3 1 c and 3 1 d located at the center. When sputtering is performed, an example of the voltage applied to the targets 3 1 a to 3 1 f is an AC voltage of -300 0 V or more with respect to the ground potential. The above description is based on the case where one slender magnet constitutes one auxiliary magnetic field forming means 1 5 a and 15 b, but the present invention is not limited to this, and a plurality of magnets may constitute one auxiliary magnetic field forming means, or each The magnet is arranged along the longitudinal direction of the target outside the region where the magnetic field forming means is arranged. In addition, the auxiliary magnetic field forming means 1 5 a and 1 5 b are adjacent to -25-

200538568 (22) 第一磁鐵42a、42f密接時,亦可一體成形該等 在上述之成膜裝置I中,即使在不移動磁 4 0 a至4 0 f與輔助磁場形成手段1 5 a、1 5 b的狀 行濺射,雖使靶材3 1 a至3 1 f的幾乎整面受到 當靶材3 1 a至3 1 f表面上的磁通密度並非均勻 密度較高的部分與較低的部分,對於因濺射所 > 減少量會產生差異。 # 爲解決該問題之本發明第2實施例之成膜 於第9圖中。該成膜裝置7係具有磁性體3 6a 之上述成膜裝置1的所有構成。成膜裝置7復具 段1 4,各磁場形成手段4 0 a至4 0 f與輔助磁場 1 5 a、1 5 b係連接於移動手段1 4,且與移動手段 動0 移動手段14係藉由未圖示之電動機,在平 3 1 a至3 1 f之表面的面內,構成爲相對於靶材3 作相對移動,因此,各磁場形成手段40a至40 f 場形成手段1 5 a、1 5 b係在平行於靶材3 1 a至3 的面內進行移動。 因此’靶材3 1 a至3 1 f之平面與磁場形成手 40f之平面間的距離並未改變。此外,各磁場 4 0 a至4 0 f與各輔助磁場形成手段1 5 a、1 5 b係固 的移動手段1 4,由於相對於移動手段1 4呈靜止 此各磁場形成手段4 0 a至4 0 f與各輔助磁場 1 5 a、1 5 b之相對位置關係並未改變。因此,靶1 $鐵。 ^形成手段 含下持續進 丨射,但是 &,在磁通 :生的膜厚 :置係顯示 :3 6f以外 有移動手 形成手段 1 4 一起移 行於靶材 1 a 至 3 1 f 與輔助磁 1 f之表面 段40a至 形成手段 定在相同 狀態,因 形成手段 才3 1 a至 -26- 200538568 (23) 3 1 f表面上的磁通密度形狀雖沒有變化,但是,磁通密度 的开狀與耙材3 1 a至3 1 f表面的相對位置關係會發生變 化。 在此,移動手段1 4之移動方向係沿著靶材3 1 a至3 1 f 的排列方向,因此,磁場形成手段40a至40f與輔助磁場 形成手段1 5 a、1 5 b係沿著靶材3 1 a至3 1 f的排列方向移 ’動。 φ 第1 〇圖(a)係表示磁場形成手段40a至40f配置在相 對應之靶材3 1 a至3 1 f的正背面位置的初期狀態,當移動 手段14移動時,如第10圖(b)所示,磁場形成手段40a 至40f會偏移相對應之靶材31a至31f的正背面位置,在 行列前頭或尾端的靶材3 1 a、31 f的端部呈從磁場形成手 段40a至4 0f突出的狀態,但是藉由移動,而使輔助磁場 形成手段1 5 a、1 5 b靠近該端部的正下方位置,結果對於 I 各靶材3 1 a至3 1 f的表面,係使磁力線從移動方向的一端 # 通至另一端爲止。 接著,就使用該成膜裝置7進行成膜的製程進行說 明。 在交換成膜完成後的基板5與新的基板5的期間,在 與上述相對應之靶材3 1 a至3 1 f鄰接的靶材3 1 a至3 1 f的 正背面位置,以磁場形成手段4 0 a至4 0 f不會進入的移動 量D使磁場形成手段40a至4 Of與輔助磁場形成手段 ]5a、15b移動,而在新的基板5的表面進行成膜時,係 使磁場形成手段40a至40f與輔助磁場形成手段i5a、15b -27-200538568 (22) When the first magnets 42a and 42f are in close contact, they can be integrally formed. In the above-mentioned film forming apparatus I, even when the magnetic field does not move 4 a to 4 0 f and the auxiliary magnetic field forming means 1 5 a, 1 5 b is sputtered, although almost the entire surface of the target 3 1 a to 3 1 f is exposed to the part where the magnetic flux density on the surface of the target 3 1 a to 3 1 f is not uniform. The difference in the amount due to sputtering ># In order to solve this problem, the film formation of the second embodiment of the present invention is shown in FIG. 9. This film forming apparatus 7 has all the configurations of the above-described film forming apparatus 1 having a magnetic body 36a. The film forming device 7 is provided with sections 14 and 4, each of the magnetic field forming means 4 a to 4 0 f and the auxiliary magnetic field 1 5 a and 1 5 b are connected to the moving means 14 and move with the moving means 0 and the moving means 14 are borrowed. A motor (not shown) is configured to move relative to the target 3 in the plane of the flat surfaces 3 1 a to 3 1 f. Therefore, each of the magnetic field forming means 40 a to 40 f and the field forming means 15 a, 1 5 b moves in a plane parallel to the targets 3 1 a to 3. Therefore, the distance between the plane of the target 3 1 a to 3 1 f and the plane of the magnetic field forming hand 40f is not changed. In addition, each of the magnetic fields 40 a to 40 f is fixed to each of the auxiliary magnetic field forming means 15 a and 15 b, and the moving means 14 is stationary with respect to the moving means 14. The relative positional relationship between 4 0 f and each auxiliary magnetic field 1 5 a, 1 5 b has not changed. So the target is $ 1 iron. ^ Forming means include continuous injection, but &, magnetic flux: raw film thickness: placement display: 3 6f There are moving hand forming means 1 4 to move to the target 1 a to 3 1 f together with the auxiliary The surface segment 40a to the forming means of the magnetic 1 f are set to the same state, and the shape of the magnetic flux density on the surface is not changed because of the forming means 3 1 a to -26- 200538568 (23) 3 1 f. The relative positional relationship between the opening shape and the surface of the rake material 3 1 a to 3 1 f will change. Here, the moving direction of the moving means 14 is along the arrangement direction of the targets 3 1 a to 3 1 f. Therefore, the magnetic field forming means 40 a to 40 f and the auxiliary magnetic field forming means 15 a, 1 5 b are along the target. The arrangement direction of the materials 3 1 a to 3 1 f moves. φ Figure 10 (a) shows the initial state where the magnetic field forming means 40a to 40f are arranged at the front and back positions of the corresponding targets 3 1 a to 3 1 f. When the moving means 14 moves, as shown in Figure 10 ( As shown in b), the magnetic field forming means 40a to 40f will be offset from the front and back positions of the corresponding targets 31a to 31f, and the ends of the targets 3 1 a and 31 f at the front or the end of the row are from the magnetic field forming means 40a. To 4 0f, but the auxiliary magnetic field forming means 1 5 a and 1 5 b are brought closer to the positions directly below the ends by moving. As a result, for the surfaces of the respective targets 3 1 a to 3 1 f, Make the magnetic field lines pass from one end # to the other end in the moving direction. Next, a film forming process using the film forming apparatus 7 will be described. During the exchange of the substrate 5 and the new substrate 5 after the completion of film formation, a magnetic field is applied to the front and back positions of the targets 3 1 a to 3 1 f adjacent to the targets 3 1 a to 3 1 f corresponding to the above. The amount of movement D that the forming means 4 0 a to 4 0 f does not enter moves the magnetic field forming means 40 a to 4 Of and the auxiliary magnetic field forming means 5 a and 15 b, and when forming a film on the surface of a new substrate 5, Magnetic field forming means 40a to 40f and auxiliary magnetic field forming means i5a, 15b -27-

200538568 (24) 相對於靶材3 1 a至3 1 f呈靜止狀態來進行濺射。 磁場的形狀與靶材3 ] a至3 1 f表面的位置關係發 化時,由於靶材3 1 a至3 1 f表面上的磁通密度較高部 發生移動,因此,靶材3 1 a至3 1 f之膜厚減少量較少 分會受到較多的濺射,相反地,膜厚減少量較多的部 受到較少的濺射。 當反覆進行磁場形成手段40a至40f與輔助磁場 手段1 5 a、1 5 b的移動與靶材3 1 a至3 1 f的濺射時, 3 1 a至3 1 f的表面會均勻減少膜厚,因此靶材3 1 a至 的使用效率較高。 此外,在第1圖的成膜裝置1中,由於在濺射部 至30f配置磁性體36a至3 6f,而使紀材31a至3 If 的磁通密度均勻,而雖然靶材3 1 a至3 1 f的膜厚均 少,但在第2實施例之成膜裝置7中,即使沒有設置 體3 6a至3 6f,亦使磁場形成手段40a至40f與輔助 形成手段1 5 a、1 5 b移動,結果使得靶材3 1 a至3 1 f 厚減少量呈均勻狀態。 以上係就磁場形成手段40a至40f與輔助磁場形 段15a、15b —起移動的情形加以說明,惟本發明並 限於此,當靶材3 1 a至3 1 f受到濺射時,若不改變各 形成手段40a至40f與輔助磁場形成手段15a、15b 之相對位置關係,而是改變相對於靶材3 1 a至3 1 f之 位置關係的話,則亦可分別移動磁場形成手段40a至 與輔助磁場形成手段1 5 a、1 5 b。 生變 分會 的部 分會 形成 靶材 3 1 f 30a 表面 勻減 磁性 磁場 的膜 成手 非侷 磁場 彼此 相對 40f -28 -200538568 (24) The sputtering is performed while the target materials 3 1 a to 3 1 f are stationary. When the relationship between the shape of the magnetic field and the position of the target 3] a to 3 1 f surface changes, the higher magnetic flux density portion on the surface of the target 3 1 a to 3 1 f moves. Therefore, the target 3 1 a The smaller the amount of film thickness reduction to 3 1 f, the more sputtering will be received. Conversely, the portion with the larger film thickness reduction will receive less sputtering. When the magnetic field forming means 40a to 40f and the auxiliary magnetic field means 1 5 a and 1 5 b are moved repeatedly and the target 3 1 a to 3 1 f is sputtered, the surface of 3 1 a to 3 1 f will uniformly reduce the film. It is thick, so the use efficiency of the targets 3 1 a to 3 is high. In addition, in the film forming apparatus 1 of FIG. 1, since the magnetic bodies 36 a to 36 f are arranged in the sputtering section to 30 f, the magnetic flux densities of the materials 31 a to 3 If are uniform, while the targets 3 1 a to 3 The film thickness of 3 1 f is small, but in the film forming apparatus 7 of the second embodiment, even if the bodies 36 a to 36 f are not provided, the magnetic field forming means 40 a to 40 f and the auxiliary forming means 1 5 a and 1 5 are used. b moves, as a result, the thickness reduction of the targets 3 1 a to 3 1 f is uniform. The above is a description of the case where the magnetic field forming means 40a to 40f and the auxiliary magnetic field sections 15a and 15b move together, but the present invention is not limited to this. When the targets 3 1 a to 3 1 f are sputtered, if they are not changed, The relative positional relationship between the forming means 40a to 40f and the auxiliary magnetic field forming means 15a, 15b, but if the positional relationship with respect to the target 3 1a to 3 1f is changed, the magnetic field forming means 40a to the auxiliary The magnetic field forming means 1 5 a, 1 5 b. Part of the variability club will form the target 3 1 f 30a The surface of the film is reduced by the magnetic magnetic field, and the non-local magnetic field is opposite each other

200538568 (25) 此外,亦可使磁場形成手段40a 3 成手段1 5 a、1 5 b靜止,而使靶材3 1 a 在不改變磁場形成手段4 0 a至4 0 f與 1 5 a、1 5 b之彼此相對位置關係而移動 3 1 a至3 1 f移動亦可。 【圖式簡單說明】 第1圖係說明本發明之一例之成膜 第2圖係說明濺射源之一例的斜視 第3圖係說明磁場形成手段與輔助 面圖。 第4圖係說明靶材與交流電源之 圖。 第5圖係膜厚分布說明圖。 > 第6圖係當配置磁場形成手段與輔 # 之磁通密度與位置關係說明圖。 第7圖係當配置磁場形成手段時之 係說明圖。 第8圖係習知技術之成膜裝置說明 第9圖係說明本發明之第2實施例 圖。 第1 0圖係說明(a)本發明之第2實 初期狀態與(b)移動後之狀態的剖面圖。 4〇f與輔助磁場形 至3 1 f移動,或是 輔助磁場形成手段 的同時,來使靶材 裝置的剖面圖。 圖。 磁場形成手段之剖 連接關係之其他例 助磁場形成手段時 磁通密度與位置關 圖。 之成膜裝置的剖面 施例之成膜裝置之 -29- 200538568 (26) 【主要元件符號說明】 1、 7、1 0 1 成膜裝置 2、 1 0 2 真空槽 3 濺射源 4 基板保持具 5、1 0 5 基板200538568 (25) In addition, the magnetic field forming means 40a 3 and the means 1 5 a and 1 5 b can be made to stand still, and the target 3 1 a can be changed without changing the magnetic field forming means 4 a a to 4 0 f and 15 a, It is also possible to move 3 1 a to 3 1 f relative to the relative positional relationship of 1 5 b. [Brief description of the drawings] Fig. 1 is a view illustrating film formation of an example of the present invention. Fig. 2 is a perspective view illustrating an example of a sputtering source. Fig. 3 is a diagram illustrating a magnetic field forming means and an auxiliary surface view. Figure 4 illustrates the target and AC power. Fig. 5 is an explanatory diagram of a film thickness distribution. > FIG. 6 is an explanatory diagram of the relationship between the magnetic flux density and the position when the magnetic field forming means and the auxiliary # are arranged. Fig. 7 is an explanatory diagram when a magnetic field forming means is arranged. Fig. 8 is a diagram illustrating a film forming apparatus of a conventional technique. Fig. 9 is a diagram illustrating a second embodiment of the present invention. Fig. 10 is a cross-sectional view illustrating (a) the initial state of the second embodiment of the present invention and (b) the state after the movement. 4of and the auxiliary magnetic field are moved to 3 1f, or the auxiliary magnetic field forming means is used to make a cross-sectional view of the target device. Illustration. Cross-section of magnetic field forming means Other examples of connection relationship When assisting magnetic field forming means, magnetic flux density vs. position. Section of the film forming device Example of film forming device -29- 200538568 (26) [Description of main component symbols] 1, 7, 1 0 1 Film forming device 2, 1 0 2 Vacuum tank 3 Sputter source 4 Substrate holding With 5, 10 5 substrate

11" 111 屏蔽 1 2、1 1 2 真空排氣系統 1 3、1 1 3 氣體供應系統 14 移動手段 1 5 a、1 5 b .輔助磁場形成手段 1 6 a、1 6b 磁轭 17a 至 17c、 117a 至 117e 電源 30a至30f 濺射部 31a 至 31f、131a 至 131e 靶材 3 3 a至3 3 f 絕緣板 35a 至 35f、135a 至 135e 電極 3 6a至3 6f 磁性體 40a至40f、140a至140e 磁場形成手段 4 1 a至4 1 f 磁轭 42a至42f 環狀磁鐵(第一磁鐵) 43a至43f 棒狀磁鐵(第二磁鐵) -30-11 " 111 Shield 1 2, 1 1 2 Vacuum exhaust system 1 3, 1 1 3 Gas supply system 14 Moving means 1 5 a, 1 5 b. Auxiliary magnetic field forming means 1 6 a, 1 6b Yoke 17a to 17c, 117a to 117e Power supply 30a to 30f Sputtering sections 31a to 31f, 131a to 131e Target 3 3a to 3 3f Insulating plates 35a to 35f, 135a to 135e Electrodes 3 6a to 3 6f Magnetic bodies 40a to 40f, 140a to 140e Magnetic field forming means 4 1 a to 4 1 f Yoke 42a to 42f Ring magnet (first magnet) 43a to 43f Rod magnet (second magnet) -30-

Claims (1)

200538568 (1) 十、申請專利範圍 1 . 一種成膜裝置,係具有:真空槽;複數個具有 邊方向的板狀靶材;以及對於前述靶材施加交流電壓的 流電源, 於前述複數個靶材之中,由相同的交流電源施加極 不同的交流電壓至不同的靶材, > 前述複數個靶材係在濺射面朝向相同方向的狀態下 Φ 將相鄰的前述靶材之長邊方向的側面配置成僅透過前述 空槽中的環境氣體而相互直接對向。 2. 如申請專利範圍第1項之成膜裝置,其中,相 對向的前述側面彼此間之距離係設爲1 mm以上、1 0mm 下。 3. 如申請專利範圍第1項或第2項之成膜裝置, 中,前述交流電源部的頻率係爲1kHz以上、l〇〇kHz ’下。 • 4. 一種成膜裝置,係具有:真空槽;以及配置於 述真空槽內部之複數個細長板狀靶材, 前述各靶材係相互平行配置成長邊方向的側面彼此 相對向的狀態, 在前述各靶材的正背面位置,沿著前述靶材的長邊 向分別配置有細長的磁場形成手段, 在比前述靶材的正背面位置還外側之配置有前述磁 形成手段的區域外側,係沿著前述靶材的長邊方向配置 細長的輔助磁場形成手段 長 交 性 J 真 互 以 其 以 —、上 刖 呈 方 場 有 -31 - 200538568 (2) 5 ·如申請專利範圍第4項之成膜裝置,其中,前述 各磁場形成手段係具有複數個磁鐵, 前述複數個磁鐵之中,與前述輔助磁場形成手段相鄰 配置之磁鐵之朝向前述靶材側的面的磁極,係設定成與前 述輔助磁場形成手段之朝向前述靶材側的面的磁極相同的 極性。 6 ·如申請專利範圍第4項或第5項之成膜裝置,# 中,具有移動手段,用於使前述磁場形成手段與前 ~ J処輔助 磁場形成手段相對於前述靶材作相對移動。200538568 (1) X. Patent application scope 1. A film-forming device having: a vacuum tank; a plurality of plate-shaped targets with side directions; and a current source for applying an AC voltage to the targets, and the targets Among the materials, very different AC voltages are applied to different targets by the same AC power source, > the plurality of targets are in a state where the sputtering surface faces the same direction Φ the long sides of the adjacent targets The side surfaces of the direction are arranged so as to directly face each other only through the ambient gas in the empty groove. 2. For example, the film-forming apparatus of the scope of patent application, wherein the distance between the opposite side surfaces is set to 1 mm or more and 10 mm or less. 3. For the film-forming device in the first or second scope of the patent application, the frequency of the AC power supply unit is 1 kHz or higher and 100 kHz or lower. • 4. A film-forming device comprising: a vacuum tank; and a plurality of elongated plate-shaped targets arranged inside the vacuum tank, wherein each of the targets is arranged parallel to each other in a direction of a growth direction, and The front and back positions of the targets are each provided with elongated magnetic field forming means along the long side of the target, and outside the area where the magnetic forming means is disposed outside the front and back positions of the target. The long and narrow auxiliary magnetic field forming means are arranged along the longitudinal direction of the aforementioned target. The long-crossing property J is true to each other, and the upper square is -31-200538568 (2) 5 In the film forming apparatus, each of the magnetic field forming means has a plurality of magnets, and among the plurality of magnets, a magnetic pole of a surface of the magnet disposed adjacent to the auxiliary magnetic field forming means toward the target side is set to be in contact with the target. The magnetic poles on the surface of the auxiliary magnetic field forming means facing the target have the same polarity. 6 · If the film-forming device in the 4th or 5th of the scope of patent application, #, there is a moving means for relative movement of the aforementioned magnetic field forming means and the auxiliary magnetic field forming means before ~ J relative to the aforementioned target. -32--32-
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