TW202317792A - Sputtering device - Google Patents

Sputtering device Download PDF

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TW202317792A
TW202317792A TW111124875A TW111124875A TW202317792A TW 202317792 A TW202317792 A TW 202317792A TW 111124875 A TW111124875 A TW 111124875A TW 111124875 A TW111124875 A TW 111124875A TW 202317792 A TW202317792 A TW 202317792A
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target
gas
magnetic
magnetic field
gap
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TWI823457B (en
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久保田清
安東靖典
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日商日新電機股份有限公司
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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
    • 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
    • C23C14/06Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the coating material
    • C23C14/08Oxides
    • C23C14/086Oxides of zinc, germanium, cadmium, indium, tin, thallium or bismuth
    • 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
    • C23C14/228Gas flow assisted PVD deposition
    • 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
    • C23C14/3407Cathode assembly for sputtering apparatus, e.g. Target
    • 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
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/02104Forming layers
    • H01L21/02365Forming inorganic semiconducting materials on a substrate
    • H01L21/02518Deposited layers
    • H01L21/02521Materials
    • H01L21/02565Oxide semiconducting materials not being Group 12/16 materials, e.g. ternary compounds
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/02104Forming layers
    • H01L21/02365Forming inorganic semiconducting materials on a substrate
    • H01L21/02612Formation types
    • H01L21/02617Deposition types
    • H01L21/02631Physical deposition at reduced pressure, e.g. MBE, sputtering, evaporation

Abstract

In the present invention, a gas is fed over the entire surface of a target. In the present invention, a vacuum container (2) of a sputtering device (1) is provided with at least one target holder (32) for holding a target (30). The target holder is provided with: a gas introduction part (51) for introducing a gas (10); and a pair of gas release ports (54) for releasing the gas into the vacuum container, the gas release ports (54) being provided at opposing positions in at least a part of the surroundings of the target.

Description

濺鍍裝置Sputtering device

本發明是有關於一種濺鍍裝置。The invention relates to a sputtering device.

自先前以來提出了各種濺鍍裝置。作為濺鍍裝置的一例,可列舉磁控濺鍍裝置。於該磁控濺鍍裝置中,藉由設置於靶的背面的磁鐵,於靶的表面形成磁場,將該磁場中的氣體電漿化,然後使電漿化後的氣體的離子與靶碰撞。藉由離子與靶碰撞,濺鍍粒子自靶飛出,藉由該粒子對與靶相向地設置的基板進行成膜。Various sputtering devices have been proposed since then. As an example of a sputtering apparatus, a magnetron sputtering apparatus is mentioned. In this magnetron sputtering apparatus, a magnetic field is formed on the surface of the target by a magnet provided on the back surface of the target, gas in the magnetic field is plasmaized, and ions of the plasmaized gas collide with the target. When the ions collide with the target, sputtering particles fly out from the target, and the particles form a film on a substrate provided to face the target.

已知於濺鍍裝置中,由於靶上的氣體的疏密,於基板上成膜的薄膜的膜厚可產生不均。於專利文獻1中揭示了抑制該不均的產生的技術的一例。於專利文獻1的濺鍍裝置中,於導入有濺鍍氣體的腔室內成組地設置有兩個靶。而且,於專利文獻1的濺鍍裝置設置有自一組靶的兩側導入反應性氣體的氣體導入口以及自一組靶之間對反應性氣體進行排氣的排氣口。 [現有技術文獻] [專利文獻] It is known that in a sputtering apparatus, the film thickness of a thin film formed on a substrate may vary due to the density of gas on a target. An example of a technique for suppressing the occurrence of this unevenness is disclosed in Patent Document 1. In the sputtering device of Patent Document 1, two targets are provided in a group in a chamber into which a sputtering gas is introduced. Moreover, the sputtering apparatus of patent document 1 is provided with the gas introduction port which introduces a reactive gas from both sides of a set of target, and the exhaust port which exhausts a reactive gas from between a set of target. [Prior art literature] [Patent Document]

[專利文獻1]日本專利特開2013-49884號公報[Patent Document 1] Japanese Patent Laid-Open No. 2013-49884

[發明所欲解決之課題] 然而,於專利文獻1的濺鍍裝置中,於一組靶中的一個靶,於該靶的一長邊側設置有氣體導入口,於該靶的與一長邊相向的長邊側設置有排氣口。因此,於該靶的與兩個長邊垂直的方向(該靶的寬度方向)上,對該靶的反應性氣體的供給量有可能變得不均勻。因此,靶的整個表面上的濺鍍粒子的飛出量有可能產生不均。其結果,於基板上形成的薄膜的膜厚有可能產生不均。 [Problem to be Solved by the Invention] However, in the sputtering device of Patent Document 1, a gas introduction port is provided on one long side of the target for one target among a set of targets, and a gas introduction port is provided on the long side opposite to the long side of the target. exhaust vent. Therefore, there is a possibility that the supply amount of the reactive gas to the target becomes non-uniform in the direction perpendicular to both long sides of the target (the width direction of the target). For this reason, there is a possibility that the amount of sputtering particles flying out may vary over the entire surface of the target. As a result, the film thickness of the thin film formed on the substrate may vary.

因此,本發明的一形態的目的在於達成一種能夠遍及靶的整個表面地供給氣體的濺鍍裝置。 [解決課題之手段] Therefore, an object of one aspect of the present invention is to achieve a sputtering device capable of supplying gas over the entire surface of a target. [Means to solve the problem]

為解決所述課題,本發明的一形態的濺鍍裝置於真空容器內對靶進行濺鍍而於基板上成膜,且所述濺鍍裝置中,所述真空容器包括保持所述靶的至少一個保持部,所述保持部包括:氣體導入部,向所述保持部導入氣體;以及一對開口部,於自鉛垂下方向觀察於所述保持部中配置所述靶的靶配置位置時,遍及所述靶配置位置的周圍的至少一部分且設置於隔著所述靶配置位置相向的位置,將導入至所述保持部內的所述氣體放出至所述真空容器內。 [發明的效果] In order to solve the above-mentioned problems, a sputtering device according to an aspect of the present invention sputters a target in a vacuum container to form a film on a substrate, and in the sputtering device, the vacuum container includes at least A holding portion, the holding portion includes: a gas introduction portion for introducing gas into the holding portion; and a pair of openings, when viewed from a vertically downward direction at a target arrangement position where the target is arranged in the holding portion, The gas introduced into the holding part is released into the vacuum container over at least a part of the periphery of the target placement position and at positions facing each other across the target placement position. [Effect of the invention]

根據本發明的一形態,可遍及靶的整個表面地供給氣體。According to one aspect of the present invention, the gas can be supplied over the entire surface of the target.

〔實施方式1〕 以下,使用圖1~圖9對本發明的一實施方式進行詳細說明。 [Embodiment 1] Hereinafter, an embodiment of the present invention will be described in detail using FIGS. 1 to 9 .

<濺鍍裝置的整體結構> 首先,使用圖1對本實施方式的濺鍍裝置1的整體結構進行說明。圖1是表示實施方式1的濺鍍裝置1的整體結構例的圖。 <Overall structure of the sputtering device> First, the overall structure of the sputtering apparatus 1 of this embodiment is demonstrated using FIG. 1. FIG. FIG. 1 is a diagram showing an example of the overall configuration of a sputtering apparatus 1 according to Embodiment 1. As shown in FIG.

如圖1所示,濺鍍裝置1是於導入濺鍍用的氣體10的真空容器2內對靶30進行濺鍍而於基板12上成膜的裝置。As shown in FIG. 1 , the sputtering apparatus 1 is an apparatus that performs sputtering on a target 30 in a vacuum container 2 into which a gas 10 for sputtering is introduced, and forms a film on a substrate 12 .

具體而言,濺鍍裝置1包括藉由真空排氣裝置4進行真空排氣的真空容器2。真空容器2電性接地,於其內部導入濺鍍用的氣體10。氣體10於藉由流量調節器8調整其流量的同時,自氣體源6經由氣體導入配管50及氣體導入部51供給至靶保持器32。然後,氣體10經由靶保持器32被導入至真空容器2。於氣體導入部51與真空容器2的上表面部3之間、及氣體導入部51與靶保持器32之間設置有絕緣部43。氣體10例如為氬氣。在進行反應性濺鍍的情況下,氣體10亦可為氬氣與活性氣體(例如氧氣、氮氣等)的混合氣體。活性氣體亦稱為反應性氣體。Specifically, the sputtering device 1 includes a vacuum container 2 that is evacuated by a vacuum exhaust device 4 . The vacuum vessel 2 is electrically grounded, and a gas 10 for sputtering is introduced into the vacuum vessel 2 . The gas 10 is supplied from the gas source 6 to the target holder 32 through the gas introduction pipe 50 and the gas introduction part 51 while adjusting the flow rate thereof by the flow regulator 8 . Then, the gas 10 is introduced into the vacuum container 2 via the target holder 32 . The insulating part 43 is provided between the gas introduction part 51 and the upper surface part 3 of the vacuum container 2, and between the gas introduction part 51 and the target holder 32. The gas 10 is, for example, argon. In the case of reactive sputtering, the gas 10 can also be a mixed gas of argon and active gas (such as oxygen, nitrogen, etc.). Reactive gases are also called reactive gases.

於真空容器2內設置有保持基板12的基板保持器14。於本實施方式中,包括基板偏置電源16,向基板保持器14施加基板偏置電壓Vs。基板偏置電壓Vs可為負的直流電壓,亦可為負的脈衝電壓、交流電壓等。另外,基板保持器14在未向基板12施加基板偏置電壓Vs的情況下,亦可電性接地。再者,40是具有真空密封功能的絕緣部。另外,基板12是藉由自靶30放出的濺鍍粒子形成薄膜的被處理物。作為基板12,可使用玻璃基板、半導體基板等,但並不限於此。A substrate holder 14 for holding a substrate 12 is provided in the vacuum vessel 2 . In this embodiment, a substrate bias power supply 16 is included to apply a substrate bias voltage Vs to the substrate holder 14 . The substrate bias voltage Vs may be a negative DC voltage, or a negative pulse voltage, AC voltage, or the like. In addition, the substrate holder 14 may also be electrically grounded when the substrate bias voltage Vs is not applied to the substrate 12 . In addition, 40 is an insulating part which has a vacuum sealing function. In addition, the substrate 12 is an object to be processed in which a thin film is formed by sputtering particles discharged from the target 30 . As the substrate 12, a glass substrate, a semiconductor substrate, or the like can be used, but is not limited thereto.

另外,於真空容器2的上表面部3,於與基板保持器14相向的位置設置有保持靶30的靶保持器(保持部)32。於圖1中,包括三個靶保持器32,但靶保持器32的數量並無限定,只要至少包括一個靶保持器32即可。藉由靶保持器32,靶30於真空容器2的內部保持於與基板12相向的位置。靶30的平面形狀例如為矩形形狀,但並不限於此,亦可為圓形形狀等。In addition, a target holder (holding portion) 32 for holding the target 30 is provided at a position facing the substrate holder 14 on the upper surface portion 3 of the vacuum vessel 2 . In FIG. 1 , three target holders 32 are included, but the number of target holders 32 is not limited as long as at least one target holder 32 is included. The target 30 is held at a position facing the substrate 12 inside the vacuum container 2 by the target holder 32 . The planar shape of the target 30 is, for example, a rectangular shape, but is not limited thereto, and may be a circular shape or the like.

靶30的材質只要與基板12上形成的膜相應即可。若示出一例,則於在基板12上形成氧化物半導體薄膜的情況下,靶30例如為由In-Ga-Zn-O(銦-鎵-鋅-氧)、或In-Sn-Zn-O(銦-錫-鋅-氧)等構成的氧化物半導體。但是,靶30的材質並不限於此。The material of the target 30 only needs to correspond to the film formed on the substrate 12 . As an example, when forming an oxide semiconductor thin film on the substrate 12, the target 30 is made of, for example, In-Ga-Zn-O (indium-gallium-zinc-oxygen) or In-Sn-Zn-O (Indium-tin-zinc-oxygen) and other oxide semiconductors. However, the material of the target 30 is not limited to this.

於靶30,經由靶保持器32連接有靶偏置電源34。靶偏置電源34向靶30供給(施加)靶偏置電壓Vt。靶偏置電壓Vt是將電漿22中的離子(於本申請案中是指正離子)引入至靶30並使其濺鍍的電壓,且例如是負的直流電壓。交流電壓例如可為13.56 MHz般的MHz級的高頻電壓,亦可為較高頻電源24的輸出(例如13.56 MHz)低的頻率(例如10 kHz~100 kHz左右)的低頻電壓。若設為低頻電壓,則容易避免與使用高頻電源24的電漿生成動作的干擾。A target bias power supply 34 is connected to the target 30 via a target holder 32 . The target bias power supply 34 supplies (applies) a target bias voltage Vt to the target 30 . The target bias voltage Vt is a voltage for introducing ions (positive ions in this application) into the target 30 in the plasma 22 to be sputtered, and is, for example, a negative DC voltage. The AC voltage may be, for example, a high-frequency voltage of the order of MHz such as 13.56 MHz, or may be a low-frequency voltage of a frequency (for example, about 10 kHz to 100 kHz) lower than the output of the frequency power supply 24 (for example, 13.56 MHz). If a low-frequency voltage is used, interference with the plasma generation operation using the high-frequency power supply 24 can be easily avoided.

進而,於真空容器2的內部配置有天線20。於本實施方式中,四根天線20以自兩側隔著由靶保持器32保持的靶30的方式相向地配置。Furthermore, an antenna 20 is arranged inside the vacuum container 2 . In the present embodiment, the four antennas 20 are arranged facing each other with the target 30 held by the target holder 32 interposed therebetween.

於各天線20,經由整合電路26連接有高頻電源24。具體而言,於各天線20的一端部連接有整合電路26,各天線20的另一端部電性接地。高頻電源24的一端亦電性接地。再者,41是具有真空密封功能的絕緣部。另外,亦可於各天線20用分別設置高頻電源24及整合電路26。A high-frequency power supply 24 is connected to each antenna 20 via an integrated circuit 26 . Specifically, an integrated circuit 26 is connected to one end of each antenna 20 , and the other end of each antenna 20 is electrically grounded. One end of the high frequency power supply 24 is also electrically grounded. In addition, 41 is an insulating part which has a vacuum sealing function. In addition, a high-frequency power supply 24 and an integrated circuit 26 may be separately provided for each antenna 20 .

高頻電源24將高頻電力Pr供給至各天線20。具體而言,藉由向各天線20並聯地供給高頻電力Pr,於靶30的表面附近產生電感耦合型的電漿22。自高頻電源24輸出的高頻電力Pr的頻率例如為一般的13.56 MHz,但並不限於此。The high-frequency power supply 24 supplies high-frequency power Pr to each antenna 20 . Specifically, by supplying high-frequency power Pr in parallel to each antenna 20 , inductively coupled plasma 22 is generated near the surface of target 30 . The frequency of the high-frequency power Pr output from the high-frequency power supply 24 is, for example, generally 13.56 MHz, but is not limited thereto.

另外,濺鍍裝置1包括控制裝置46。控制裝置46對濺鍍裝置1的各部分進行統一控制。特別是控制裝置46對自高頻電源24及靶偏置電源34的電力供給進行控制。另外,控制裝置46對流量調節器8進行控制,而對導入至真空容器2的氣體10的流量進行控制。In addition, the sputtering device 1 includes a control device 46 . The control device 46 collectively controls each part of the sputtering device 1 . In particular, the control device 46 controls the power supply from the high-frequency power supply 24 and the target bias power supply 34 . In addition, the control device 46 controls the flow regulator 8 to control the flow rate of the gas 10 introduced into the vacuum vessel 2 .

再者,與流量調節器8連接的氣體導入配管50、氣體絕緣配管501及氣體導入部51設置於各個靶保持器32,但於圖1中省略了其圖示。另外,高頻電源24經由整合電路26而連接於各天線20,但於圖1中省略了其圖示。進而,靶偏置電源34連接於各個靶保持器32中保持的靶30,但於圖1中省略了其圖示。In addition, the gas introduction pipe 50 connected to the flow rate regulator 8, the gas insulation pipe 501, and the gas introduction part 51 are provided in each target holder 32, However, It abbreviate|omits illustration in FIG. In addition, the high-frequency power supply 24 is connected to each antenna 20 via an integrated circuit 26 , but its illustration is omitted in FIG. 1 . Furthermore, the target bias power supply 34 is connected to the target 30 held by each target holder 32 , but its illustration is omitted in FIG. 1 .

<真空容器的上表面部附近的結構> 接著,使用圖1對真空容器2的上表面部3附近的具體結構進行詳細說明。於上表面部3附近,主要設置有 ·於靶30的表面附近產生電漿22的天線20、 ·保持靶30的靶保持器32。 <Structure near the upper surface of the vacuum container> Next, the specific structure of the vicinity of the upper surface part 3 of the vacuum vessel 2 is demonstrated in detail using FIG. 1. FIG. In the vicinity of the upper surface part 3, there are mainly Antenna 20 for generating plasma 22 near the surface of target 30, • Target holder 32 holding target 30 .

(天線) 如圖1所示,天線20配置於真空容器2內部的靶保持器32的附近(具體而言,由靶保持器32保持的靶30的表面附近)。於本實施方式中,如圖1所示,多根天線20以自兩側隔著由靶保持器32保持的靶30的方式、例如以沿著矩形形狀的靶30的邊的方式配置。 (antenna) As shown in FIG. 1 , the antenna 20 is disposed near the target holder 32 inside the vacuum chamber 2 (specifically, near the surface of the target 30 held by the target holder 32 ). In the present embodiment, as shown in FIG. 1 , the plurality of antennas 20 are arranged across the target 30 held by the target holder 32 from both sides, for example, along the sides of the rectangular target 30 .

藉由如此配置多根天線20,能夠以與靶30的整個表面相向的方式產生電漿22。藉此,能夠對靶30的整個表面進行濺鍍,能夠提高靶30的利用效率。但是,若不考慮這一點,則例如亦可將一根天線20以沿著靶30的單側的邊的方式配置。By arranging the plurality of antennas 20 in this way, plasma 22 can be generated so as to face the entire surface of target 30 . Thereby, sputtering can be performed on the entire surface of the target 30, and the utilization efficiency of the target 30 can be improved. However, if this point is not considered, for example, one antenna 20 may be arranged along one side of the target 30 .

另外,各天線20連接於整合電路26。各天線20可為中央堵塞的實心結構,亦可為中空結構(例:管狀或筒狀)。在為中空結構的情況下,亦可設為於其內部設置冷卻水路,藉由使冷卻水流動而對各天線20進行冷卻的水冷結構。另外,各天線20亦可為於天線導體的中途插入電容器的結構。In addition, each antenna 20 is connected to an integrated circuit 26 . Each antenna 20 can be a solid structure blocked in the center, or a hollow structure (eg tubular or cylindrical). In the case of a hollow structure, a cooling water channel may be provided inside, and each antenna 20 may be cooled by a water-cooling structure in which cooling water flows. In addition, each antenna 20 may have a structure in which a capacitor is inserted in the middle of the antenna conductor.

再者,天線20的形狀並不限於以上所述的形狀,整體可為棒狀,亦可為U字狀、C字狀、線圈狀等。另外,天線20的形狀亦可設為與靶30的平面形狀相應的形狀。例如,在靶30的平面形狀為圓形形狀的情況下,亦可將天線20的平面形狀設為圓形形狀。Furthermore, the shape of the antenna 20 is not limited to the above-mentioned shapes, and the overall shape may be a rod shape, or a U-shape, a C-shape, a coil shape, and the like. In addition, the shape of the antenna 20 may be a shape corresponding to the planar shape of the target 30 . For example, when the planar shape of the target 30 is a circular shape, you may make the planar shape of the antenna 20 into a circular shape.

另外,天線20成為不依賴於其結構或形狀而天線導體均收納於絕緣性構件的內側的結構。In addition, the antenna 20 has a structure in which all antenna conductors are accommodated inside the insulating member regardless of its structure or shape.

以上所述的天線20的結構或形狀只不過是一例,天線20只要為能夠產生電漿22的結構或形狀即可。The structure and shape of the antenna 20 described above are merely examples, and the antenna 20 may have a structure or shape capable of generating the plasma 22 .

另外,與向靶30供給靶偏置電壓Vt獨立地,對天線20供給高頻電力Pr。具體而言,控制裝置46(參照圖1)對向靶30供給靶偏置電壓Vt的靶偏置電源34以及向天線20供給高頻電力Pr的高頻電源24進行獨立的控制。In addition, high-frequency power Pr is supplied to the antenna 20 independently of supplying the target bias voltage Vt to the target 30 . Specifically, the control device 46 (see FIG. 1 ) independently controls the target bias power supply 34 that supplies the target bias voltage Vt to the target 30 and the high-frequency power supply 24 that supplies high-frequency power Pr to the antenna 20 .

(靶保持器的結構) 靶保持器32由規定靶保持器32的結構的結構構件、於靶30附近導入氣體10的氣體構件、以及於靶30的表面附近形成磁場的磁路構件構成。另外,靶保持器32由向靶保持器32施加電壓的電極構件、用於使電極構件絕緣的絕緣構件、以及對靶保持器32進行冷卻的冷卻構件構成。 (Structure of Target Holder) The target holder 32 is composed of structural members defining the structure of the target holder 32 , a gas member for introducing the gas 10 near the target 30 , and a magnetic circuit member for forming a magnetic field near the surface of the target 30 . In addition, the target holder 32 is constituted by an electrode member for applying a voltage to the target holder 32 , an insulating member for insulating the electrode member, and a cooling member for cooling the target holder 32 .

使用圖2~圖8對以上所述的靶保持器32的各構件進行說明。圖2是實施方式1的靶保持器32的圖1中的A-A向視圖,且是組裝了靶保持器32的狀態下的俯視圖。圖3是實施方式1的靶保持器32的圖1中的B-B向視圖,且是組裝了靶保持器32的狀態下的仰視圖。圖4是實施方式1的靶保持器32的圖1中的C-C向視圖。圖5是實施方式1的靶保持器32的圖1中的D-D向視圖。圖6是實施方式1的靶保持器32的圖1中的E-E向視圖。圖7是實施方式1的靶保持器32的圖2中的F-F剖面圖。圖8是實施方式1的靶保持器32的圖2中的G-G剖面圖。Each member of the above-mentioned target holder 32 is demonstrated using FIGS. 2-8. FIG. 2 is a view taken along the line A-A in FIG. 1 of the target holder 32 according to Embodiment 1, and is a plan view in a state where the target holder 32 is assembled. FIG. 3 is a view taken along the line B-B in FIG. 1 of the target holder 32 according to Embodiment 1, and is a bottom view of the state where the target holder 32 is assembled. FIG. 4 is a view taken along line C-C in FIG. 1 of the target holder 32 according to the first embodiment. FIG. 5 is a D-D arrow view in FIG. 1 of the target holder 32 according to the first embodiment. FIG. 6 is a view taken along the line E-E in FIG. 1 of the target holder 32 according to the first embodiment. FIG. 7 is a sectional view taken along line F-F in FIG. 2 of the target holder 32 according to the first embodiment. FIG. 8 is a G-G sectional view in FIG. 2 of the target holder 32 according to the first embodiment.

再者,於圖3中,為了便於說明,省略了由靶保持器32保持的靶30的圖示。In addition, in FIG. 3, illustration of the target 30 held by the target holder 32 is abbreviate|omitted for convenience of description.

(靶保持器的結構構件) 首先,作為靶保持器32的結構構件,例如,如圖7及圖8所示,包括靶主體321以及背板322。 (Structural member of target holder) First, as structural members of the target holder 32 , for example, as shown in FIGS. 7 and 8 , a target main body 321 and a back plate 322 are included.

靶主體321是規定靶保持器32的各種構件的構件。於靶主體321形成有規定各種構件的槽及孔、或者用於組裝各種構件的槽及孔。各種構件的功能及結構將於後面敘述。The target main body 321 is a member that defines various members of the target holder 32 . Grooves and holes for defining various members, or grooves and holes for assembling various members are formed in the target main body 321 . The functions and structures of various components will be described later.

背板322是用來安裝靶30的板。將於背板322的與基板保持器14相向之側的表面上安裝(配置)靶30的位置稱為靶配置位置30a(亦參照圖3及圖6)。背板322配置於靶主體321的下部。於背板322構成有氣體構件的一部分(例如,氣體放出口54)。The back plate 322 is a plate on which the target 30 is mounted. The position where the target 30 is mounted (arranged) on the surface of the back plate 322 facing the substrate holder 14 is referred to as a target arrangement position 30 a (also refer to FIGS. 3 and 6 ). The back plate 322 is disposed on the lower portion of the target body 321 . A part of the gas member (for example, the gas outlet 54 ) is formed on the back plate 322 .

靶主體321及背板322的自鉛垂下方向觀察時的形狀(平面形狀)只要與成為安裝對象的靶30的形狀一致地設計即可。例如,若安裝的靶30的平面形狀為矩形形狀,則靶主體321及背板322的平面形狀只要設計為矩形形狀即可。The shapes (planar shapes) of the target main body 321 and the back plate 322 as viewed from the vertically downward direction may be designed to match the shape of the target 30 to be mounted. For example, if the planar shape of the target 30 to be attached is a rectangular shape, the planar shape of the target body 321 and the back plate 322 may be designed as a rectangular shape.

在靶主體321及背板322的平面形狀為矩形形狀的情況下,靶主體321及背板322的角部亦可為經倒角的形狀。於本實施方式中,靶主體321及背板322的平面形狀為矩形形狀,但靶主體321及背板322的角部成為R形狀。該形狀起因於設置靶主體321及背板322的上表面部3的加工上的限制、及於靶主體321及背板322的邊緣部產生異常放電的風險的降低等理由。但是,若不考慮這一點,則靶主體321及背板322的平面形狀亦可為角部未經倒角的矩形形狀。When the planar shapes of the target body 321 and the back plate 322 are rectangular, the corners of the target body 321 and the back plate 322 may be chamfered. In this embodiment, although the planar shape of the target main body 321 and the back plate 322 is a rectangular shape, the corner|angular part of the target main body 321 and the back plate 322 becomes R shape. The reason for this shape is to limit the processing of the upper surface portion 3 where the target body 321 and the back plate 322 are placed, and to reduce the risk of abnormal discharges occurring at the edge portions of the target body 321 and the back plate 322 . However, if this point is not considered, the planar shape of the target body 321 and the back plate 322 may be a rectangular shape without chamfering at the corners.

再者,於本說明書中,在靶主體321的平面形狀、背板322的平面形狀(靶配置位置30a的平面形狀)、及靶30的平面形狀表現為矩形形狀的情況下,應注意具有以下兩種含義。即,於本說明書中,該矩形形狀除了包含(i)角部未經倒角的形狀(通常含義上的矩形形狀)之外,亦包含(ii)矩形的角部經倒角的形狀。Furthermore, in this specification, when the planar shape of the target main body 321, the planar shape of the back plate 322 (the planar shape of the target placement position 30a), and the planar shape of the target 30 are rectangular, it should be noted that the following Two meanings. That is, in this specification, the rectangular shape includes (i) a shape in which the corners are not chamfered (rectangular shape in a general sense) and (ii) a shape in which the corners of the rectangle are chamfered.

於本實施方式中,靶主體321及背板322的長度方向沿Y軸方向(例如,於圖7及圖8中為紙面的進深方向)延伸。即,例如,如圖3所示,靶配置位置30a的長度方向(長邊)沿Y軸方向延伸,靶30以靶30的長度方向(長邊)沿Y軸方向延伸的方式安裝於背板322。In this embodiment, the longitudinal directions of the target main body 321 and the back plate 322 extend along the Y-axis direction (for example, in FIG. 7 and FIG. 8 , the depth direction of the paper surface). That is, for example, as shown in FIG. 3 , the longitudinal direction (long side) of the target arrangement position 30a extends along the Y-axis direction, and the target 30 is attached to the back plate so that the longitudinal direction (long side) of the target 30 extends along the Y-axis direction. 322.

(靶保持器的氣體構件) 如圖7所示,靶保持器32的氣體構件包括:氣體導入配管50、氣體絕緣配管501、氣體導入部51、氣體路徑(主路徑)52、氣體路徑蓋521、節流孔522、氣體分支路徑(分支路徑)53、以及氣體放出口(開口部)54。 (Gas member of target holder) As shown in FIG. 7 , the gas components of the target holder 32 include: a gas introduction pipe 50 , a gas insulation pipe 501 , a gas introduction part 51 , a gas path (main path) 52 , a gas path cover 521 , an orifice 522 , and a gas branch. path (branch path) 53 , and gas discharge port (opening portion) 54 .

氣體導入配管50是將自氣體源6供給的氣體10導入至靶保持器32內的路徑(管路),且連接於氣體源6與氣體導入部51之間(亦參照圖1)。另外,如圖1所示,於氣體導入配管50的中途設置有流量調節器8。另外,氣體絕緣配管501是用於使氣體導入配管50與氣體導入部51絕緣的配管。The gas introduction pipe 50 is a path (pipeline) for introducing the gas 10 supplied from the gas source 6 into the target holder 32 , and is connected between the gas source 6 and the gas introduction part 51 (see also FIG. 1 ). In addition, as shown in FIG. 1 , a flow regulator 8 is provided in the middle of the gas introduction pipe 50 . In addition, the gas insulating pipe 501 is a pipe for insulating the gas introduction pipe 50 and the gas introduction part 51 .

氣體導入部51是形成於靶主體321的、向靶保持器32內導入氣體10的路徑,且將氣體導入配管50與氣體路徑52連通。針對每個靶保持器32設置有一個氣體導入部51,如圖2所示,設置於靶保持器32的端部。The gas introduction part 51 is a path formed in the target main body 321 to introduce the gas 10 into the target holder 32 , and communicates the gas introduction pipe 50 and the gas path 52 . One gas introduction portion 51 is provided for each target holder 32 , and is provided at an end of the target holder 32 as shown in FIG. 2 .

氣體路徑52是形成於靶主體321的、接受自氣體導入部51導入的氣體10並使其向氣體分支路徑53流動的路徑,且與氣體導入部51及氣體分支路徑53連通。於本實施方式中,氣體路徑52是設置於靶主體321的上表面側、且自鉛垂下方向觀察時為靶主體321的中央附近,沿靶主體321的長度方向延伸地形成的路徑(參照圖6)。自氣體導入部51導入的氣體10藉由氣體路徑52而於靶主體321的長度方向上被分散。The gas path 52 is formed in the target main body 321 to receive the gas 10 introduced from the gas introduction part 51 to flow to the gas branch path 53 , and communicates with the gas introduction part 51 and the gas branch path 53 . In this embodiment, the gas path 52 is provided on the upper surface side of the target body 321, and is formed near the center of the target body 321 when viewed from a vertically downward direction, and is formed to extend along the longitudinal direction of the target body 321 (see FIG. 6). The gas 10 introduced from the gas introduction part 51 is dispersed in the longitudinal direction of the target body 321 by the gas path 52 .

氣體路徑蓋521是氣體路徑52的蓋。藉由氣體路徑蓋521,可降低氣體10向氣體導入部51及氣體分支路徑53以外流出的可能性(參照圖5)。另外,氣體路徑蓋521包括使來自氣體導入部51的氣體10向氣體路徑52流動的節流孔522。藉由在氣體路徑蓋521設置節流孔522,可提高較節流孔522更靠上游部的氣體壓力。The gas passage cover 521 is a cover for the gas passage 52 . The possibility of the gas 10 flowing out of the gas introduction part 51 and the gas branch path 53 can be reduced by the gas path cover 521 (see FIG. 5 ). In addition, the gas passage cover 521 includes an orifice 522 through which the gas 10 from the gas introduction part 51 flows into the gas passage 52 . By providing the orifice 522 in the gas path cover 521, the gas pressure at the upstream portion of the orifice 522 can be increased.

此處,氣體導入部51藉由利用絕緣部43按入氣體導入部的凸緣部分而具有真空密封功能。另外,氣體導入部51連接於氣體路徑蓋521,與靶偏置電壓Vt成為相同電位。另外,氣體導入配管50與氣體導入部51藉由氣體絕緣配管501而絕緣。因此,藉由在氣體導入配管50及氣體導入部51產生的高頻的電位、以及氣體導入配管50及氣體導入部51中的氣體10的壓力,於氣體10中可發生放電。為了不發生此種放電,規定氣體導入配管50的長度,並且於氣體路徑蓋521設置有節流孔522。Here, the gas introduction part 51 has a vacuum sealing function by pressing the flange part of the gas introduction part with the insulating part 43 . In addition, the gas introduction part 51 is connected to the gas passage cover 521, and has the same potential as the target bias voltage Vt. In addition, the gas introduction pipe 50 and the gas introduction part 51 are insulated by the gas insulation pipe 501 . Therefore, discharge can be generated in the gas 10 by the high-frequency potential generated in the gas introduction pipe 50 and the gas introduction part 51 and the pressure of the gas 10 in the gas introduction pipe 50 and the gas introduction part 51 . In order not to generate such a discharge, the length of the gas introduction pipe 50 is specified, and an orifice 522 is provided in the gas passage cover 521 .

氣體分支路徑53是形成於靶主體321的、將自氣體路徑52導入的氣體10導入至氣體放出口54的路徑,且與氣體路徑52及氣體放出口54連通。於本實施方式中,氣體分支路徑53在靶主體321的寬度方向(X軸方向)上隔著氣體路徑52相向的位置形成有多個(參照圖6)。The gas branch path 53 is a path formed in the target body 321 for introducing the gas 10 introduced from the gas path 52 to the gas outlet 54 , and communicates with the gas path 52 and the gas outlet 54 . In the present embodiment, a plurality of gas branch paths 53 are formed at positions facing each other across the gas path 52 in the width direction (X-axis direction) of the target body 321 (see FIG. 6 ).

具體而言,如圖6所示,氣體分支路徑53的一端於沿著氣體路徑52的長度方向(Y軸方向)延伸的氣體路徑52的兩側面的各個上與氣體路徑52連通。另外,氣體分支路徑53的另一端於靶主體321的下表面且為於靶主體321的寬度方向上隔著靶配置位置30a相向的位置上,與氣體放出口54連通。Specifically, as shown in FIG. 6 , one end of the gas branch path 53 communicates with the gas path 52 on each of both side surfaces of the gas path 52 extending along the longitudinal direction (Y-axis direction) of the gas path 52 . In addition, the other end of the gas branch path 53 is located on the lower surface of the target body 321 at a position opposite to the target arrangement position 30 a in the width direction of the target body 321 , and communicates with the gas discharge port 54 .

氣體放出口54是形成於背板322的、將自氣體分支路徑53導入的氣體10放出至真空容器2的內部的開口部,且與氣體分支路徑53連通。於本實施方式中,於自鉛垂下方向觀察時,氣體放出口54遍及靶配置位置30a的相向的長邊的整體而設置有多個(參照圖6)。另外,於本實施方式中,多個氣體放出口54於靶配置位置30a的各長邊大致均等地設置,且以設置於各長邊的氣體放出口54相互相向的方式設置。因此,由氣體導入部51導入的氣體10以自靶30的兩長邊側大致均勻地遍及靶30的整個表面的方式被供給至安裝於靶配置位置30a的靶30。因此,與自靶30的單邊側供給氣體10的情況相比,可向靶30的整個表面大致均勻地供給氣體10。The gas outlet 54 is an opening formed in the back plate 322 for releasing the gas 10 introduced from the gas branch path 53 into the vacuum container 2 , and communicates with the gas branch path 53 . In the present embodiment, when viewed from the vertically downward direction, a plurality of gas discharge ports 54 are provided over the entire length of the opposing long sides of the target arrangement position 30 a (see FIG. 6 ). In addition, in this embodiment, the some gas discharge port 54 is provided in each long side of the target arrangement position 30a substantially equally, and is provided so that the gas discharge port 54 provided in each long side may oppose each other. Therefore, the gas 10 introduced by the gas introduction part 51 is supplied to the target 30 attached to the target arrangement position 30a so that it may spread substantially uniformly over the whole surface of the target 30 from both long sides of the target 30. Therefore, compared with the case where the gas 10 is supplied from one side of the target 30 , the gas 10 can be supplied substantially uniformly over the entire surface of the target 30 .

再者,氣體放出口54的配置位置及個數並不限於上述,只要調整為將自氣體放出口54放出的氣體10大致均勻地供給至靶30的整個表面即可。In addition, the arrangement position and number of the gas discharge ports 54 are not limited to the above, and may be adjusted so that the gas 10 discharged from the gas discharge ports 54 is supplied substantially uniformly to the entire surface of the target 30 .

例如,氣體放出口54可遍及靶配置位置30a的兩短邊的整體而設置,亦可設置於靶配置位置30a的長邊側及短邊側的各者。但是,設置於靶配置位置30a的長邊側更容易使氣體10大致均勻地供給至靶30的整個表面。For example, the gas discharge port 54 may be provided over the entirety of both short sides of the target arrangement position 30a, or may be provided on each of the long side and the short side of the target arrangement position 30a. However, it is easier to supply the gas 10 substantially uniformly to the entire surface of the target 30 if it is provided on the long side of the target arrangement position 30 a.

另外,一對氣體放出口54未必需要以相向的方式設置。例如,於靶配置位置30a的相向的邊彼此,氣體放出口54的數量亦可不同。另外,氣體放出口54各自的開口的大小亦可不同。進而,一個氣體放出口54亦可沿著靶30的邊而設置。In addition, the pair of gas discharge ports 54 does not necessarily have to be provided so as to face each other. For example, the number of gas discharge ports 54 may be different between sides facing each other at the target arrangement position 30a. In addition, the size of each opening of the gas discharge port 54 may be different. Furthermore, one gas discharge port 54 may be provided along the side of the target 30 .

即,氣體放出口54只要以將氣體10大致均勻地供給至靶30的整個表面的方式遍及靶配置位置30a的周圍的至少一部分且設置於隔著靶配置位置30a相向的位置即可。That is, the gas outlets 54 may extend over at least a part of the periphery of the target arrangement position 30 a and be provided at positions facing each other across the target arrangement position 30 a so as to supply the gas 10 substantially uniformly over the entire surface of the target 30 .

此處,氣體分支路徑53的粗細(YZ剖面中的剖面積)較氣體路徑52的粗細(XZ剖面中的剖面積)小(參照圖6、圖7)。因此,於氣體分支路徑53中流動的氣體10較於氣體路徑52中流動的氣體10更難以流動。因此,可提高氣體路徑52中的氣體10的壓力,其結果,可遍及氣體路徑52的整體使該壓力均等化。因此,可向各氣體分支路徑53大致均等地供給氣體10。另外,導入至靶保持器32內的氣體10的流量被調節為恆定。因此,藉由使氣體分支路徑53的粗細較氣體路徑52的粗細小,且使氣體放出口54的粗細較氣體分支路徑53的粗細小,可提高自氣體放出口54放出的氣體10的流速。因此,能夠以於靶30的整個表面上疏密的部分變少的方式將氣體10分散。Here, the thickness of the gas branch path 53 (cross-sectional area in the YZ cross section) is smaller than the thickness (cross-sectional area in the XZ cross-section) of the gas path 52 (see FIGS. 6 and 7 ). Therefore, the gas 10 flowing in the gas branch path 53 is more difficult to flow than the gas 10 flowing in the gas path 52 . Therefore, the pressure of the gas 10 in the gas path 52 can be increased, and as a result, the pressure can be equalized over the entire gas path 52 . Therefore, the gas 10 can be supplied substantially equally to each gas branch path 53 . In addition, the flow rate of the gas 10 introduced into the target holder 32 is adjusted to be constant. Therefore, by making the gas branch path 53 smaller than the gas path 52, and making the gas outlet 54 smaller than the gas branch path 53, the flow rate of the gas 10 discharged from the gas outlet 54 can be increased. Therefore, it is possible to disperse the gas 10 so as to reduce the density of the entire surface of the target 30 .

(靶保持器的電極構件及絕緣構件) 如圖2及圖3所示,作為靶保持器32的電極構件,包括電極71以及陽極72。另外,如圖8所示,靶保持器32的絕緣構件包括絕緣襯套421、第一絕緣板422、以及第二絕緣板423。 (Electrode member and insulating member of the target holder) As shown in FIGS. 2 and 3 , an electrode 71 and an anode 72 are included as electrode members of the target holder 32 . In addition, as shown in FIG. 8 , the insulating member of the target holder 32 includes an insulating bush 421 , a first insulating plate 422 , and a second insulating plate 423 .

電極71是將靶偏置電壓Vt輸入至靶保持器32的電極。電極71針對每個靶保持器32設置有一個電極71,如圖2所示,與氣體導入部51鄰接地設置於靶保持器32的端部。經由電極71,靶主體321、背板322及靶30帶電為靶偏置電壓Vt。The electrode 71 is an electrode for inputting a target bias voltage Vt to the target holder 32 . Electrode 71 One electrode 71 is provided for each target holder 32 , and as shown in FIG. 2 , it is provided at an end portion of the target holder 32 adjacent to the gas introduction portion 51 . Through the electrode 71, the target main body 321, the back plate 322, and the target 30 are charged to a target bias voltage Vt.

絕緣襯套421是使於上表面部3固定靶主體321的螺栓絕緣的襯套。於本實施方式中,絕緣襯套421沿著靶保持器32的長度方向(Y軸方向),於隔著磁場強度調整板61相向的位置設置有多個(參照圖2)。The insulating bush 421 is a bush that insulates bolts that fix the target body 321 to the upper surface portion 3 . In the present embodiment, a plurality of insulating bushes 421 are provided at positions facing each other along the longitudinal direction (Y-axis direction) of the target holder 32 via the magnetic field intensity adjustment plate 61 (see FIG. 2 ).

第一絕緣板422是設置於上表面部3與靶主體321之間的、與設置靶30的平面平行的平面上的絕緣構件。具體而言,第一絕緣板422設置於氣體路徑蓋521與第一磁性板63之間。The first insulating plate 422 is an insulating member provided between the upper surface portion 3 and the target body 321 on a plane parallel to the plane on which the target 30 is installed. Specifically, the first insulating plate 422 is disposed between the gas path cover 521 and the first magnetic plate 63 .

第二絕緣板423是設置於上表面部3與靶主體321之間的、與設置靶30的平面垂直的平面上的絕緣構件。第二絕緣板423以包圍靶主體321的四角的方式設置。The second insulating plate 423 is an insulating member provided between the upper surface portion 3 and the target body 321 on a plane perpendicular to the plane on which the target 30 is placed. The second insulating plate 423 is provided to surround the four corners of the target body 321 .

作為絕緣構件的絕緣襯套421、第一絕緣板422、第二絕緣板423具有使帶電為靶偏置電壓Vt的靶主體321及背板322與電性接地的真空容器2及上表面部3絕緣的功能。The insulating bushing 421 as an insulating member, the first insulating plate 422, and the second insulating plate 423 have the target main body 321 and the back plate 322 charged to the target bias voltage Vt, and the vacuum vessel 2 and the upper surface portion 3 electrically grounded. Insulation function.

陽極72是用於與於後述的第三磁性板67的端部間形成的平行磁場一起於靶30附近捕捉因靶30處的離子碰撞而產生的電子(二次電子)的電極。藉此,可提高靶30附近的電漿22的密度。再者,陽極72電性接地。The anode 72 is an electrode for capturing electrons (secondary electrons) generated by ion collision at the target 30 near the target 30 together with a parallel magnetic field formed between ends of the third magnetic plate 67 described later. Thereby, the density of the plasma 22 near the target 30 can be increased. Furthermore, the anode 72 is electrically grounded.

來自靶30的二次電子被平行磁場捕捉,因此可降低二次電子入射至基板12的表面的可能性。因此,可降低基板12的溫度上升的可能性。另外,藉由將平行磁場的磁場強度設定得小,即便二次電子未被平行磁場捕捉到,亦不會發生回旋加速器(註冊商標)運動而消失。二次電子例如入射至周邊的壁上或者藉由空間中的再結合而消失。因此,可減小二次電子對基板12的表面附近的電漿22的高密度化造成的影響。Since the secondary electrons from the target 30 are captured by the parallel magnetic field, the possibility of the secondary electrons entering the surface of the substrate 12 can be reduced. Therefore, the possibility of temperature rise of the substrate 12 can be reduced. In addition, by setting the magnetic field intensity of the parallel magnetic field to be small, even if the secondary electrons are not captured by the parallel magnetic field, they will not disappear due to cyclotron (registered trademark) motion. The secondary electrons, for example, are incident on the surrounding walls or disappear by recombination in space. Therefore, the influence of the secondary electrons on the increase in density of the plasma 22 near the surface of the substrate 12 can be reduced.

於本實施方式中,如圖3及圖8所示,陽極72設置於靶配置位置30a的附近,且具有呈與靶配置位置30a的外緣類似的形狀的環狀形狀。於本實施方式中,陽極72是以覆蓋氣體放出口54、及配置於靶配置位置30a的靶30的外緣的方式設置。另外,陽極72以與靶30的外緣具有間隙的方式設置於靶保持器32。因此,可使於氣體放出口54放出的氣體10自該間隙向靶30擴散。另外,藉由陽極72,後述的第三磁性板67不與電漿22相接。因此,可降低藉由第三磁性板67與電漿22相接而於真空容器2內部產生雜質的風險。In this embodiment, as shown in FIG. 3 and FIG. 8 , the anode 72 is provided near the target placement position 30 a and has an annular shape similar to the outer edge of the target placement position 30 a. In the present embodiment, the anode 72 is provided so as to cover the gas outlet 54 and the outer edge of the target 30 arranged at the target arrangement position 30 a. In addition, the anode 72 is provided on the target holder 32 with a gap from the outer edge of the target 30 . Therefore, the gas 10 discharged from the gas discharge port 54 can be diffused toward the target 30 from the gap. In addition, the third magnetic plate 67 described later is not in contact with the plasma 22 due to the anode 72 . Therefore, the risk of impurities being generated inside the vacuum container 2 due to the contact between the third magnetic plate 67 and the plasma 22 can be reduced.

(關於磁路) 此處,於說明靶保持器32的磁路構件之前,對磁路進行說明。磁路是由磁鐵以及被磁鐵磁化的磁構件構成的生成磁場的電路。 (about the magnetic circuit) Here, the magnetic circuit will be described before describing the magnetic circuit members of the target holder 32 . The magnetic circuit is a circuit that generates a magnetic field and is composed of a magnet and a magnetic member magnetized by the magnet.

磁鐵是藉由磁動勢生成磁場,使磁通流向磁鐵的外部的物質。磁構件是使由磁鐵生成的磁通通過的構件。作為磁構件,可列舉磁軛(軛鐵)、鐵等磁導率高的強磁性體等。A magnet is a substance that generates a magnetic field by magnetomotive force, and causes magnetic flux to flow to the outside of the magnet. The magnetic member is a member through which the magnetic flux generated by the magnet passes. Examples of the magnetic member include ferromagnetic materials with high magnetic permeability such as yokes (iron yokes) and iron.

於磁路中亦可形成作為間隙的空隙。空隙可形成於形成磁路的兩個磁構件之間。於空隙中插入磁導率較磁構件小的物質(例如,空氣)。因此,空隙中的磁阻較磁構件中的磁阻大。因此,藉由對設置於磁路中的空隙的寬度(兩個磁構件之間的間隔)進行調整,可改變磁路整體的磁阻。A void as a gap may also be formed in the magnetic circuit. A gap may be formed between two magnetic members forming a magnetic circuit. A substance with a lower magnetic permeability than the magnetic member (for example, air) is inserted into the gap. Therefore, the reluctance in the air gap is greater than that in the magnetic member. Therefore, by adjusting the width of the gap (interval between two magnetic members) provided in the magnetic circuit, the magnetic resistance of the entire magnetic circuit can be changed.

(靶保持器的磁路構件) 如圖8所示,靶保持器32的磁路構件是形成以上所述的磁路的構件,包括磁鐵65以及磁構件。作為該磁構件,包括:磁場強度調整板(磁調整構件)61、磁路徑螺栓(固定構件)62、第一磁性板63、磁鐵保持部64、第二磁性板66、以及第三磁性板67。 (Magnetic circuit member of target holder) As shown in FIG. 8 , the magnetic circuit member of the target holder 32 is a member forming the above-mentioned magnetic circuit, and includes a magnet 65 and a magnetic member. As the magnetic member, a magnetic field intensity adjustment plate (magnetic adjustment member) 61 , a magnetic path bolt (fixing member) 62 , a first magnetic plate 63 , a magnet holding portion 64 , a second magnetic plate 66 , and a third magnetic plate 67 are included. .

磁場強度調整板61是設置於向真空容器2的外部的大氣側露出的上表面部3(即,靶保持器32的上表面部320)的磁構件。磁場強度調整板61是沿靶保持器32的長度方向延伸的一對磁構件(參照圖2)。而且,於一對磁場強度調整板61之間形成有空隙61a。即,空隙61a由磁場強度調整板61規定。另外,於磁場強度調整板61形成有多個貫通磁路徑螺栓62並沿空隙61a的寬度方向(X軸方向)延伸的長孔61b(參照圖2及圖9)。圖9是圖2中的H部的放大圖。The magnetic field intensity adjustment plate 61 is a magnetic member provided on the upper surface portion 3 (that is, the upper surface portion 320 of the target holder 32 ) exposed to the outside air side of the vacuum container 2 . The magnetic field intensity adjustment plates 61 are a pair of magnetic members extending in the longitudinal direction of the target holder 32 (see FIG. 2 ). Furthermore, a gap 61 a is formed between the pair of magnetic field intensity adjustment plates 61 . That is, the gap 61 a is defined by the magnetic field intensity adjustment plate 61 . In addition, a plurality of elongated holes 61 b extending in the width direction (X-axis direction) of the air gap 61 a are formed in the magnetic field strength adjustment plate 61 (see FIGS. 2 and 9 ) passing through the magnetic path bolts 62 . FIG. 9 is an enlarged view of part H in FIG. 2 .

磁路徑螺栓62是將各個磁場強度調整板61固定於靶保持器32的磁構件。具體而言,使磁路徑螺栓62穿過磁場強度調整板61的長孔61b,固定於第一磁性板63,藉此將磁場強度調整板61固定於靶保持器32。The magnetic path bolt 62 is a magnetic member that fixes each magnetic field intensity adjustment plate 61 to the target holder 32 . Specifically, the magnetic path bolt 62 is passed through the elongated hole 61 b of the magnetic field strength adjustment plate 61 and fixed to the first magnetic plate 63 , thereby fixing the magnetic field strength adjustment plate 61 to the target holder 32 .

長孔61b的寬度方向(X軸方向)的長度較磁路徑螺栓62的軸徑大。因此,可變更長孔61b中的磁路徑螺栓62的貫通位置。即,可按照與長孔61b的寬度方向上的長度相應的量,變更磁場強度調整板61相對於靶保持器32的固定位置。因此,藉由調整磁場強度調整板61的固定位置,可調整空隙61a的寬度。如此,磁場強度調整板61及磁路徑螺栓62作為調整空隙61a的寬度的調整機構發揮功能。The length of the long hole 61 b in the width direction (X-axis direction) is larger than the shaft diameter of the magnetic path bolt 62 . Therefore, the penetrating position of the magnetic path bolt 62 in the elongated hole 61b is variable. That is, the fixed position of the magnetic field intensity adjustment plate 61 with respect to the target holder 32 can be changed by the amount corresponding to the length of the long hole 61b in the width direction. Therefore, by adjusting the fixed position of the magnetic field strength adjustment plate 61, the width of the gap 61a can be adjusted. In this way, the magnetic field intensity adjustment plate 61 and the magnetic path bolt 62 function as an adjustment mechanism for adjusting the width of the air gap 61 a.

再者,於本實施方式中,磁場強度調整板61兩者形成有長孔61b,但並不限於此。例如,亦可僅於其中一個磁場強度調整板61形成長孔61b,另一個磁場強度調整板61固定於上表面部3。即便在此情況下,亦可變更其中一個磁場強度調整板61相對於另一個磁場強度調整板61的位置,因此可調整空隙61a的寬度。Furthermore, in this embodiment, both the magnetic field intensity adjustment plates 61 are formed with the elongated holes 61b, but the present invention is not limited thereto. For example, the long hole 61 b may be formed in only one of the magnetic field intensity adjustment plates 61 , and the other magnetic field intensity adjustment plate 61 may be fixed to the upper surface portion 3 . Even in this case, the position of one of the magnetic field intensity adjustment plates 61 relative to the other magnetic field intensity adjustment plate 61 can be changed, so the width of the gap 61a can be adjusted.

第一磁性板63是沿靶保持器32的長度方向延伸的一對磁構件(參照圖4)。第一磁性板63分別以與兩個磁場強度調整板61對應的方式固定於第一絕緣板422與上表面部3之間。The first magnetic plates 63 are a pair of magnetic members extending in the longitudinal direction of the target holder 32 (see FIG. 4 ). The first magnetic plates 63 are respectively fixed between the first insulating plate 422 and the upper surface portion 3 so as to correspond to the two magnetic field intensity adjustment plates 61 .

磁鐵保持部64是保持磁鐵65的一對磁構件。磁鐵保持部64沿靶保持器32的長度方向延伸,可於各個磁鐵保持部64中保持多個磁鐵65(參照圖4)。磁鐵保持部64分別設置於與第一磁性板63分別相向且接近的位置。再者,磁鐵保持部64與第一磁性板63亦可接觸。即,亦可於第一磁性板63的一部分設置保持磁鐵65的部分。The magnet holder 64 is a pair of magnetic members that hold the magnet 65 . The magnet holding parts 64 extend along the longitudinal direction of the target holder 32 , and can hold a plurality of magnets 65 in each of the magnet holding parts 64 (see FIG. 4 ). The magnet holders 64 are respectively provided at positions facing and close to the first magnetic plates 63 . Furthermore, the magnet holding portion 64 may also be in contact with the first magnetic plate 63 . That is, a portion holding the magnet 65 may be provided on a part of the first magnetic plate 63 .

磁鐵65是具有可使磁構件磁化的磁強度(磁動勢)的構件。作為磁鐵65,例如使用半永久磁鐵,在此情況下,可廉價且容易地構成所期望的磁路。作為磁鐵65,於其中一個磁鐵保持部64及另一個磁鐵保持部64中使用不同磁極的磁鐵。例如,其中一個磁鐵保持部64保持N極的磁鐵65,另一個磁鐵保持部64保持S極的磁鐵65。The magnet 65 is a member having a magnetic strength (magnetomotive force) capable of magnetizing the magnetic member. As the magnet 65, for example, a semi-permanent magnet is used, and in this case, a desired magnetic circuit can be formed inexpensively and easily. As the magnet 65 , magnets with different magnetic poles are used for one of the magnet holding portions 64 and the other magnet holding portion 64 . For example, one of the magnet holding parts 64 holds the magnet 65 of the N pole, and the other magnet holding part 64 holds the magnet 65 of the S pole.

第二磁性板66是分別與磁鐵保持部64接觸地設置的一對磁性構件,且沿靶保持器32的長度方向延伸(參照圖5)。第二磁性板66分別固定於第二絕緣板423與上表面部3之間。再者,只要可形成磁路,則第二磁性板66亦可設置於與磁鐵保持部64隔開的位置。The second magnetic plates 66 are a pair of magnetic members provided in contact with the magnet holders 64 , respectively, and extend in the longitudinal direction of the target holder 32 (see FIG. 5 ). The second magnetic plates 66 are respectively fixed between the second insulating plates 423 and the upper surface portion 3 . Furthermore, as long as a magnetic circuit can be formed, the second magnetic plate 66 may be provided at a position spaced from the magnet holding portion 64 .

第三磁性板67是分別與第二磁性板66接觸地設置的一對磁性構件,且沿靶保持器32的長度方向延伸。第三磁性板67藉由將陽極72固定於第二磁性板66的固定構件(例:螺栓),而固定於陽極72與第二磁性板66之間(參照圖8)。另外,當自鉛垂下方向觀察時,第三磁性板67配置於隔著靶30相向的位置,所述靶30配置於靶配置位置30a。即,第三磁性板67設置為與陽極72一併覆蓋氣體放出口54。The third magnetic plates 67 are a pair of magnetic members respectively provided in contact with the second magnetic plates 66 , and extend in the lengthwise direction of the target holder 32 . The third magnetic plate 67 is fixed between the anode 72 and the second magnetic plate 66 by fixing the anode 72 to the fixing member (for example, a bolt) of the second magnetic plate 66 (see FIG. 8 ). Moreover, the 3rd magnetic plate 67 is arrange|positioned at the position which opposes across the target 30 arrange|positioned at the target arrangement|positioning position 30a, seeing from a vertical downward direction. That is, the third magnetic plate 67 is provided so as to cover the gas outlet 54 together with the anode 72 .

如以上所述,由磁場強度調整板61、磁路徑螺栓62、第一磁性板63、磁鐵保持部64、磁鐵65、第二磁性板66、第三磁性板67形成一個磁路。即,磁鐵65的磁動勢出現於各第三磁性板67的端部,於第三磁性板67的端部間形成平行磁場。As described above, one magnetic circuit is formed by the magnetic field intensity adjustment plate 61 , the magnetic path bolt 62 , the first magnetic plate 63 , the magnet holder 64 , the magnet 65 , the second magnetic plate 66 , and the third magnetic plate 67 . That is, the magnetomotive force of the magnet 65 appears at the ends of the third magnetic plates 67 , and a parallel magnetic field is formed between the ends of the third magnetic plates 67 .

(靶保持器的冷卻構件) 如圖2、圖3及圖7所示,靶保持器32的冷卻構件是對靶30進行水冷的構件,且包括冷卻水口81以及冷卻水路徑82。 (Cooling member of target holder) As shown in FIGS. 2 , 3 and 7 , the cooling member of the target holder 32 is a member for water cooling the target 30 and includes a cooling water port 81 and a cooling water path 82 .

冷卻水口81藉由對靶保持器32供給/排出冷卻水來對靶保持器32進行冷卻。如圖2所示,針對每個靶保持器32設置有冷卻水口81,且設置於靶保持器32中的與設置有氣體導入部51的端部為相反側的端部。作為冷卻水,可使用水以外的冷媒。The cooling water port 81 cools the target holder 32 by supplying/discharging cooling water to the target holder 32 . As shown in FIG. 2 , a cooling water port 81 is provided for each target holder 32 , and is provided at the end of the target holder 32 opposite to the end where the gas introduction part 51 is provided. As the cooling water, a refrigerant other than water can be used.

冷卻水路徑82是於靶主體321的下表面沿著靶主體321的長邊方向而設置的U字狀的槽(參照圖3及圖7)。使自冷卻水口81的供水口供給的冷卻水呈U字狀流動,自冷卻水口81的排水口排水,藉此對靶保持器32進行冷卻。The cooling water path 82 is a U-shaped groove provided on the lower surface of the target body 321 along the longitudinal direction of the target body 321 (see FIGS. 3 and 7 ). The target holder 32 is cooled by making the cooling water supplied from the water supply port of the cooling water port 81 flow in a U-shape and draining it from the drain port of the cooling water port 81 .

<用於膜厚分佈的均勻化的方法> 為了使於基板12上成膜的薄膜的膜厚分佈均勻化, ·靶30的表面上的氣體10的分佈(壓力分佈)的均勻化 ·靶30間的氣體10的分佈的均勻化 ·靶30的表面上的平行磁場的形成區域 成為重要的要素之一。對與該些相關的說明及其方法進行詳細說明。 <Method for homogenizing film thickness distribution> In order to make the film thickness distribution of the thin film formed on the substrate 12 uniform, · Homogenization of the distribution (pressure distribution) of the gas 10 on the surface of the target 30 - Uniform distribution of gas 10 between targets 30 ・A region where a parallel magnetic field is formed on the surface of the target 30 become one of the important elements. Descriptions related to these and their methods will be described in detail.

(靶的表面上的氣體的分佈) 於本實施方式中,濺鍍裝置1自隔著靶配置位置30a而設置於靶保持器32的長度方向上的多個氣體放出口54將氣體10放出至真空容器2內,藉此進行濺鍍。如上所述,陽極72設置成於與靶30之間具有間隙,且覆蓋靶30的外緣。即,陽極72於靶30的下方,以向靶30側突出的方式設置。因此,自氣體放出口54放出的氣體10朝向陽極72的突出方向、即朝向靶30的中央區域向靶30的表面放出。因此,濺鍍裝置1可使氣體10遍及靶30的整個表面地分佈。 (distribution of gas on the surface of the target) In the present embodiment, the sputtering apparatus 1 discharges the gas 10 into the vacuum container 2 from a plurality of gas discharge ports 54 provided in the longitudinal direction of the target holder 32 across the target arrangement position 30a, thereby performing sputtering. . As described above, the anode 72 is provided with a gap between the target 30 and covers the outer edge of the target 30 . That is, the anode 72 is provided below the target 30 so as to protrude toward the target 30 side. Therefore, the gas 10 released from the gas discharge port 54 is discharged toward the surface of the target 30 toward the protruding direction of the anode 72 , that is, toward the central region of the target 30 . Therefore, the sputtering apparatus 1 can distribute the gas 10 over the entire surface of the target 30 .

而且,藉由流量調節器8調整氣體10的流量,可使氣體10以大致均勻的濃度遍及靶30的整個表面地分佈。因此,可使濺鍍粒子大致均勻地自靶30放出,可使於基板12上成膜的薄膜的膜厚大致均勻。即,可使基板12的膜厚分佈均勻化。Furthermore, by adjusting the flow rate of the gas 10 by the flow regulator 8, the gas 10 can be distributed over the entire surface of the target 30 at a substantially uniform concentration. Therefore, the sputtering particles can be emitted from the target 30 substantially uniformly, and the film thickness of the thin film formed on the substrate 12 can be made substantially uniform. That is, the film thickness distribution of the substrate 12 can be made uniform.

(靶間的氣體的分佈) 於本實施方式中,為了對大型基板進行濺鍍,設置有多個靶保持器32。於各靶保持器32如上述般設置有多個氣體放出口54。因此,於各靶保持器32中,遍及靶30的整個表面地供給自氣體放出口54放出的氣體10。另外,各氣體導入部51等管路(配管)被設計為,藉由流量調節器8對向各氣體導入部51供給的總流量進行調節,並且氣體10於各氣體導入部51中大致均等地流動。因此,於各靶保持器32中,可使來自氣體放出口54的氣體10的放出量均勻化。因此,由於可使各靶保持器32中的氣體10的分佈均勻化,因此可使與各靶保持器32相向的基板12的膜厚分佈均勻化。再者,於各靶保持器32亦可各別地設置流量調節器8。在此情況下,亦可使於各氣體導入部51中流動的氣體10的流量均勻化。 (distribution of gas between targets) In the present embodiment, in order to perform sputtering on a large substrate, a plurality of target holders 32 are provided. A plurality of gas outlets 54 are provided in each target holder 32 as described above. Therefore, the gas 10 discharged from the gas discharge port 54 is supplied to each target holder 32 over the entire surface of the target 30 . In addition, the pipelines (pipes) such as each gas introduction part 51 are designed so that the total flow rate supplied to each gas introduction part 51 is adjusted by the flow rate regulator 8, and the gas 10 is distributed approximately equally in each gas introduction part 51. flow. Therefore, in each target holder 32 , the discharge amount of the gas 10 from the gas discharge port 54 can be made uniform. Therefore, since the distribution of the gas 10 in each target holder 32 can be made uniform, the film thickness distribution of the substrate 12 facing each target holder 32 can be made uniform. In addition, the flow regulator 8 may be provided in each target holder 32 individually. Also in this case, the flow rate of the gas 10 flowing in each gas introduction part 51 can be made uniform.

另外,於本實施方式中,濺鍍裝置1於靶30的兩長邊側自接近靶30的位置進行氣體10向靶30的放出。因此,相較於自一組靶30的兩側導入反應性氣體,自一組靶30之間對反應性氣體進行排氣的結構(例:專利文獻1的濺鍍裝置),可縮短靶30間的距離。即,可減小靶保持器32間的間距。因此,可減小不與靶30相向的基板12的區域,因此可進一步使基板12的膜厚分佈均勻化。In addition, in the present embodiment, the sputtering apparatus 1 discharges the gas 10 to the target 30 from a position close to the target 30 on both long side sides of the target 30 . Therefore, compared with the structure in which reactive gas is introduced from both sides of a set of targets 30 and the reactive gas is exhausted from between a set of targets 30 (for example: the sputtering device of Patent Document 1), the target 30 can be shortened. distance between. That is, the pitch between the target holders 32 can be reduced. Therefore, since the area of the substrate 12 that does not face the target 30 can be reduced, the film thickness distribution of the substrate 12 can be further made uniform.

進而,於本實施方式中,設置有一個真空排氣裝置4。另外,真空排氣裝置4設置於與基板保持器14不同的位置,所述基板保持器14設置於真空容器2的底面部的中央部。因此,各靶保持器32與真空排氣裝置4的距離互不相同。其結果,各靶保持器32的配置位置處的真空排氣的速度不同。Furthermore, in this embodiment, one vacuum exhaust device 4 is provided. In addition, the vacuum evacuation device 4 is provided at a different position from the substrate holder 14 provided at the center of the bottom surface of the vacuum container 2 . Therefore, the distances between the respective target holders 32 and the vacuum evacuation device 4 are different from each other. As a result, the evacuation speed differs at the arrangement position of each target holder 32 .

考慮到這一點,為了使氣體10向各靶30的分佈進一步均勻化,例如亦可針對每個靶保持器32設置流量調節器8。藉此,可根據各靶保持器32的配置位置處的真空排氣的速度,來調節氣體10的流量。因此,無論真空排氣裝置4的配置位置如何,均可使氣體10向各靶30的分佈均勻化,其結果,可使基板12的膜厚分佈均勻化。In consideration of this point, in order to further uniformize the distribution of the gas 10 to each target 30 , for example, a flow regulator 8 may be provided for each target holder 32 . Thereby, the flow rate of the gas 10 can be adjusted according to the speed of vacuum exhaust at the position where each target holder 32 is arranged. Therefore, regardless of the arrangement position of the evacuation device 4 , the distribution of the gas 10 to each target 30 can be made uniform, and as a result, the film thickness distribution of the substrate 12 can be made uniform.

或者,亦可將與真空排氣裝置4連接的多個真空配管配置於相對於靶保持器32群對稱的位置。例如,所述真空配管亦可設置於真空容器2的相向的兩個側壁、即沿著靶保持器32的長度方向延伸的兩個側壁。另外,例如,所述真空配管亦可於真空容器2的底部設置於所述兩個側壁的各自附近。在此情況下,可減小各靶保持器32的配置位置處的真空排氣的速度的差異,因此可使氣體10向各靶30的分佈均勻化。另外,藉由後述的實施方式2的結構亦可獲得相同的效果。Alternatively, a plurality of vacuum pipes connected to the vacuum evacuation device 4 may be arranged at symmetrical positions with respect to the target holder 32 group. For example, the vacuum piping may be provided on two opposing side walls of the vacuum container 2 , that is, two side walls extending along the longitudinal direction of the target holder 32 . In addition, for example, the vacuum piping may be provided at the bottom of the vacuum container 2 near each of the two side walls. In this case, since the difference in the speed of vacuum exhaust at the arrangement position of each target holder 32 can be reduced, the distribution of the gas 10 to each target 30 can be made uniform. In addition, the same effect can also be obtained by the structure of Embodiment 2 mentioned later.

(磁路帶來的效果) 如圖8所示,一對第三磁性板67配置於靶30的附近,於一對第三磁性板67分別形成有磁極。因此,至少於與靶30的整個表面相向的位置,可形成具有與該表面大致平行的磁力線的成分的磁場分佈(平行磁場)。因此,可效率良好地捕捉因靶30處的離子碰撞而產生的電子(二次電子)。 (The effect brought by the magnetic circuit) As shown in FIG. 8 , a pair of third magnetic plates 67 is arranged near the target 30 , and magnetic poles are formed on the pair of third magnetic plates 67 , respectively. Therefore, at least at a position facing the entire surface of the target 30 , a magnetic field distribution (parallel magnetic field) having a component of magnetic force lines substantially parallel to the surface can be formed. Therefore, electrons (secondary electrons) generated by ion collisions at the target 30 can be efficiently captured.

另外,藉由在與靶30的整個表面相向的位置形成平行磁場,能夠遍及靶30的整個表面一致地捕捉電子。藉由如上所述般配置多個天線20,能夠以與靶30的整個表面相向的方式產生電漿22。但是,即便在此情況下,電漿22的密度亦有可能於靶30的表面局部存在化。藉由形成所述平行磁場而對電子進行捕捉,可抑制所述電漿22的密度的局部存在化。因此,能夠一致地對靶30的整個表面進行濺鍍。因此,可使基板12的膜厚分佈均勻化。In addition, electrons can be captured uniformly over the entire surface of the target 30 by forming a parallel magnetic field at a position facing the entire surface of the target 30 . By arranging a plurality of antennas 20 as described above, plasma 22 can be generated so as to face the entire surface of target 30 . However, even in this case, the density of the plasma 22 may be localized on the surface of the target 30 . By trapping electrons by forming the parallel magnetic field, localization of the density of the plasma 22 can be suppressed. Therefore, sputtering can be uniformly performed on the entire surface of the target 30 . Therefore, the film thickness distribution of the substrate 12 can be made uniform.

由於電子於大範圍內自靶30飛出,因此形成於第三磁性板67的磁極越遠離靶30的表面,捕捉該電子的概率(捕捉率、收率)越下降,並且濺鍍裝置1的結構變大。藉由將第三磁性板67設置於靶30附近,可於提高電子的收率的同時達成設置了第三磁性板67時的濺鍍裝置1的小型化。Since electrons fly out from the target 30 in a wide range, the farther the magnetic poles formed on the third magnetic plate 67 are from the surface of the target 30, the lower the probability (capture rate, yield) of capturing the electrons, and the sputtering device 1 The structure becomes larger. By providing the third magnetic plate 67 in the vicinity of the target 30 , the yield of electrons can be improved while reducing the size of the sputtering apparatus 1 when the third magnetic plate 67 is provided.

再者,磁路所形成的磁場強度(磁通密度)小於產生磁控管放電的強度。於濺鍍裝置1中,由於利用天線20產生電漿22,因此無需產生如發生磁控管放電般的高強度的磁場。Furthermore, the magnetic field strength (magnetic flux density) formed by the magnetic circuit is smaller than the strength of the magnetron discharge. In the sputtering apparatus 1 , since the antenna 20 generates the plasma 22 , it is not necessary to generate a high-intensity magnetic field such as a magnetron discharge.

(磁路對磁場的調整) 另外,平行磁場的強度是藉由磁鐵65的磁強度以及形成於一對磁場強度調整板61之間的空隙61a的寬度來調整。如上所述,於磁場強度調整板61形成有沿磁場強度調整板61的寬度方向延伸的長孔61b。因此,於長孔61b的範圍內,藉由變更磁路徑螺栓62對磁場強度調整板61進行固定的位置,可調整空隙61a的寬度。因此,可調整空隙61a中的磁阻,因此可調整磁路的磁阻。因此,由於可調整平行磁場的強度,因此可遍及靶30的整個表面一致地捕捉電子。再者,空隙61a的寬度只要調整為可形成平行磁場的程度的寬度即可,所述平行磁場具有能夠遍及靶30的整個表面一致地捕捉電子的程度的強度。 (Adjustment of the magnetic field by the magnetic circuit) In addition, the strength of the parallel magnetic field is adjusted by the magnetic strength of the magnet 65 and the width of the gap 61 a formed between the pair of magnetic field strength adjustment plates 61 . As described above, the long hole 61 b extending in the width direction of the magnetic field strength adjustment plate 61 is formed in the magnetic field strength adjustment plate 61 . Therefore, within the range of the elongated hole 61b, the width of the gap 61a can be adjusted by changing the position where the magnetic path bolt 62 fixes the magnetic field intensity adjustment plate 61 . Therefore, the reluctance in the air gap 61a can be adjusted, and thus the reluctance of the magnetic circuit can be adjusted. Therefore, since the intensity of the parallel magnetic field can be adjusted, electrons can be uniformly captured over the entire surface of the target 30 . It should be noted that the width of the gap 61 a may be adjusted to a width capable of forming a parallel magnetic field having a strength sufficient to capture electrons uniformly over the entire surface of the target 30 .

另外,於本實施方式中,可針對每個靶保持器32調整空隙61a的寬度。因此,於各靶保持器32中,可遍及靶30的整個表面一致地捕捉電子。In addition, in the present embodiment, the width of the gap 61 a can be adjusted for each target holder 32 . Therefore, electrons can be captured uniformly over the entire surface of the target 30 in each target holder 32 .

另外,於空隙61a中插入具有與磁構件不同的磁導率的物質(於本實施方式中為空氣)。因此,藉由在磁路中形成空隙61a,可形成具有與僅由磁鐵及磁構件形成的磁路不同的磁阻的磁路。In addition, a substance (in this embodiment, air) having a magnetic permeability different from that of the magnetic member is inserted into the gap 61 a. Therefore, by forming the air gap 61a in the magnetic circuit, it is possible to form a magnetic circuit having a magnetic resistance different from a magnetic circuit formed only by magnets and magnetic members.

再者,由於空氣的磁導率較磁構件的磁導率小,因此空隙61a具有大的磁阻。因此,空隙61a的寬度越大,平行磁場的強度越小,且其強度分佈越差。在平行磁場的強度分佈變差的情況下,於靶30的整個表面無法形成平行磁場,有可能於電子的捕捉中產生不均。因此,考慮到充滿空隙61a的物質(此處為空氣)的磁導率,空隙61a的寬度設定為於與靶30的整個表面相向的位置可形成平行磁場的程度的寬度。Furthermore, since the magnetic permeability of air is smaller than that of the magnetic member, the air gap 61a has a large magnetic resistance. Therefore, the larger the width of the air gap 61a, the smaller the intensity of the parallel magnetic field, and the worse the intensity distribution thereof. When the intensity distribution of the parallel magnetic field deteriorates, the parallel magnetic field cannot be formed on the entire surface of the target 30, and unevenness may occur in capturing electrons. Therefore, the width of the gap 61 a is set to such a degree that a parallel magnetic field can be formed at a position facing the entire surface of the target 30 in consideration of the magnetic permeability of the substance (here, air) filling the gap 61 a.

(濺鍍裝置的小型化) 於本實施方式中,於靶保持器32的內部設置有磁路及氣體放出口54。另外,隨著於靶保持器32的內部設置氣體放出口54,氣體路徑52及氣體分支路徑53亦設置於靶保持器32的內部。因此,無需於靶保持器32間構築氣體10的路徑,因此能夠以多個靶保持器32相互鄰接的方式將多個靶保持器32安裝於上表面部3。因此,可使濺鍍裝置1小型化。另外,藉由濺鍍裝置1的小型化,可減小不與靶30相向的基板12的區域。因此,可使基板12的膜厚分佈進一步均勻化。 (miniaturization of sputtering equipment) In this embodiment, a magnetic circuit and a gas discharge port 54 are provided inside the target holder 32 . In addition, as the gas outlet 54 is provided inside the target holder 32 , the gas path 52 and the gas branch path 53 are also provided inside the target holder 32 . Therefore, since it is not necessary to construct the path of the gas 10 between the target holders 32, several target holders 32 can be attached to the upper surface part 3 so that several target holders 32 may adjoin each other. Therefore, the size of the sputtering apparatus 1 can be reduced. Moreover, the area|region of the board|substrate 12 which does not oppose the target 30 can be reduced by downsizing the sputtering apparatus 1. FIG. Therefore, the film thickness distribution of the substrate 12 can be further uniformed.

(小結) 如上所述,根據以上所述的氣體放出口54的配置位置,可使靶30的表面上的氣體10的分佈均勻化。即,根據該配置位置,可遍及靶30的整個表面一致地供給氣體10。因此,可使基板12的膜厚分佈均勻化。另外,藉由調整以上所述的空隙61a的寬度,可調整平行磁場的強度,以便可遍及靶30的整個表面一致地捕捉電子。藉由該調整亦可使基板12的膜厚分佈均勻化。 (summary) As described above, the distribution of the gas 10 on the surface of the target 30 can be made uniform according to the arrangement positions of the gas discharge ports 54 described above. That is, according to this arrangement position, the gas 10 can be uniformly supplied over the entire surface of the target 30 . Therefore, the film thickness distribution of the substrate 12 can be made uniform. In addition, by adjusting the width of the gap 61a described above, the strength of the parallel magnetic field can be adjusted so that electrons can be uniformly captured over the entire surface of the target 30 . The film thickness distribution of the substrate 12 can also be made uniform by this adjustment.

另外,為了調整基板12的膜厚分佈,可於真空容器2的外部利用流量調節器8進行氣體10的流量調整、及磁場強度調整板61的配置位置的調整(空隙61a的調整)。因此,可在不將真空容器2打開的情況下容易地調整基板12的膜厚分佈。In addition, in order to adjust the film thickness distribution of the substrate 12 , the flow rate of the gas 10 and the position of the magnetic field intensity adjustment plate 61 (adjustment of the gap 61 a ) can be adjusted by using the flow regulator 8 outside the vacuum vessel 2 . Therefore, the film thickness distribution of the substrate 12 can be easily adjusted without opening the vacuum container 2 .

〔實施方式2〕 以下,使用圖10及圖11對其他實施方式進行詳細說明。再者,為了便於說明,對與所述實施方式中所說明的構件具有相同功能的構件標註相同的符號,並不重覆其說明。 [Embodiment 2] Hereinafter, other embodiments will be described in detail using FIGS. 10 and 11 . In addition, for convenience of description, the same code|symbol is attached|subjected to the member which has the same function as the member demonstrated in the said embodiment, and the description is not repeated.

於實施方式1中,藉由一個真空排氣裝置4集中地對氣體10進行排氣,但於實施方式2中,濺鍍裝置1亦包括多個排氣口(排氣部)55。圖10是表示實施方式2的真空容器2內的詳細結構的剖面圖。圖11是實施方式2的靶保持器32的圖10中的H-H向視圖,且是組裝了靶保持器32的狀態下的仰視圖。In Embodiment 1, the gas 10 is collectively exhausted by one vacuum exhaust device 4 , but in Embodiment 2, the sputtering apparatus 1 also includes a plurality of exhaust ports (exhaust parts) 55 . FIG. 10 is a cross-sectional view showing the detailed structure inside the vacuum vessel 2 according to the second embodiment. FIG. 11 is a view taken along the line H-H in FIG. 10 of the target holder 32 according to Embodiment 2, and is a bottom view in a state where the target holder 32 is assembled.

如圖10所示,排氣口55是與對真空容器2內進行真空排氣的真空排氣裝置連接,對自氣體放出口54放出的氣體10進行排氣的排氣口。排氣口55於上表面部3設置於與靶保持器32鄰接的位置。於本實施方式中,設置於多個靶保持器32之間。如圖11所示,排氣口55沿著靶保持器32的長度方向設置有多個。As shown in FIG. 10 , the exhaust port 55 is connected to a vacuum exhaust device for evacuating the inside of the vacuum container 2 , and is an exhaust port for exhausting the gas 10 released from the gas discharge port 54 . The exhaust port 55 is provided at a position adjacent to the target holder 32 on the upper surface portion 3 . In the present embodiment, it is provided between a plurality of target holders 32 . As shown in FIG. 11 , a plurality of exhaust ports 55 are provided along the longitudinal direction of the target holder 32 .

藉由如上所述般於靶保持器32附近包括排氣口55,產生自氣體放出口54放出的氣體10朝向排氣口55流動的氣流。藉由該氣流的產生,可使靶30的整個表面上的氣體10的分佈更均勻化。另外,排氣口55設置於多個靶保持器32間,因此於各靶保持器32中產生的氣流容易變得均勻。因此,使各靶30處的氣體10的分佈均勻化變得容易,結果可使基板12的膜厚分佈均勻化。By including the exhaust port 55 near the target holder 32 as described above, a gas flow in which the gas 10 discharged from the gas discharge port 54 flows toward the exhaust port 55 is generated. The distribution of the gas 10 over the entire surface of the target 30 can be made more uniform by the generation of this gas flow. In addition, since the exhaust port 55 is provided between the plurality of target holders 32, the airflow generated in each target holder 32 becomes easy to become uniform. Therefore, it becomes easy to make the distribution of the gas 10 uniform at each target 30 , and as a result, the film thickness distribution of the substrate 12 can be made uniform.

再者,排氣口55亦可於與靶保持器32鄰接的位置沿著靶保持器32的短邊方向而設置。即,排氣口55只要設置於靶保持器32周圍的至少一部分即可。排氣口55沿著靶保持器32的長度方向而設置時可使靶30的整個表面上的氣體10的分佈更均勻化。另外,排氣口55亦可為沿著靶保持器32的長邊方向或短邊方向而設置的一個開口部。In addition, the exhaust port 55 may be provided along the short-side direction of the target holder 32 at a position adjacent to the target holder 32 . That is, the exhaust port 55 has only to be provided in at least a part of the periphery of the target holder 32 . When the exhaust port 55 is provided along the longitudinal direction of the target holder 32 , the distribution of the gas 10 on the entire surface of the target 30 can be made more uniform. In addition, the exhaust port 55 may be a single opening provided along the long-side direction or the short-side direction of the target holder 32 .

另外,靶保持器32亦可為於真空容器2的內部僅設置一個的結構。即便在此情況下,藉由在靶保持器32的鄰接的位置如上所述般設置排氣口55,亦可使靶30的整個表面上的氣體10的分佈更均勻化。即,藉由在一個靶保持器32的附近設置排氣口55,可使靶30的整個表面上的氣體10的分佈更均勻化。In addition, only one target holder 32 may be provided in the inside of the vacuum container 2 . Even in this case, by providing the exhaust ports 55 as described above at positions adjacent to the target holder 32 , the distribution of the gas 10 over the entire surface of the target 30 can be made more uniform. That is, by providing the exhaust port 55 in the vicinity of one target holder 32, the distribution of the gas 10 over the entire surface of the target 30 can be made more uniform.

另外,於本實施方式中,亦可不於真空容器2直接設置真空排氣裝置4。另外,亦可為於濺鍍中,真空排氣裝置4停止,僅藉由排氣口55進行排氣的結構。在該些結構的情況下,不使用真空排氣裝置4而僅自排氣口55對氣體10進行排氣。因此,可降低各靶保持器32中的氣體10的排氣速度的不均,因此可使各靶30處的氣體10的分佈更均勻化。另外,與各靶保持器32對應地設置流量調節器8,即便不藉由各流量調節器8精度良好地調整氣體10的流量,亦可使各靶30處的氣體10的分佈更均勻化。In addition, in this embodiment, the vacuum exhaust device 4 may not be provided directly in the vacuum container 2 . In addition, during the sputtering, the vacuum evacuation device 4 is stopped, and the evacuation is performed only through the exhaust port 55 . In the case of these structures, the gas 10 is exhausted only from the exhaust port 55 without using the vacuum exhaust device 4 . Therefore, since the variation in the exhaust velocity of the gas 10 in each target holder 32 can be reduced, the distribution of the gas 10 at each target 30 can be made more uniform. In addition, the flow regulators 8 are provided corresponding to the target holders 32 , so that the distribution of the gas 10 at the targets 30 can be made more uniform even if the flow rates of the gas 10 are not adjusted accurately by the flow regulators 8 .

〔實施方式3〕 以下,將使用圖12對其他實施方式進行詳細說明。再者,為了便於說明,對與所述實施方式中所說明的構件具有相同功能的構件標註相同的符號,並不重覆其說明。 [Embodiment 3] Hereinafter, other embodiments will be described in detail using FIG. 12 . In addition, for convenience of description, the same code|symbol is attached|subjected to the member which has the same function as the member demonstrated in the said embodiment, and the description is not repeated.

圖12是實施方式1的磁場強度調整板61及實施方式3的磁場強度調整板610的概略圖。圖12的符號1201表示磁場強度調整板61,符號1202表示磁場強度調整板610。於實施方式1中,一對磁場強度調整板61分別由一個板構成。因此,形成於磁場強度調整板61之間的空隙61a相對於磁場強度調整板61的長度方向具有一樣的寬度(長度L)。另一方面,於實施方式3中,一對磁場強度調整板610(磁調整構件)分別於磁場強度調整板610的長邊方向上被分割成多個分區。FIG. 12 is a schematic diagram of the magnetic field intensity adjustment plate 61 of the first embodiment and the magnetic field intensity adjustment plate 610 of the third embodiment. Reference numeral 1201 in FIG. 12 indicates the magnetic field intensity adjustment plate 61 , and reference numeral 1202 indicates the magnetic field intensity adjustment plate 610 . In Embodiment 1, each of the pair of magnetic field strength adjustment plates 61 is composed of one plate. Therefore, the gap 61 a formed between the magnetic field strength adjustment plates 61 has the same width (length L) with respect to the longitudinal direction of the magnetic field strength adjustment plates 61 . On the other hand, in Embodiment 3, a pair of magnetic field intensity adjustment plates 610 (magnetic adjustment members) are each divided into a plurality of sections in the longitudinal direction of the magnetic field intensity adjustment plates 610 .

具體而言,一對磁場強度調整板610是由多個成對的磁場板構成的磁場板群。如圖12所示,於本實施方式中,一對磁場強度調整板610於磁場強度調整板610的長度方向上具有三組成對的磁場板611、612及613。第一組磁場板611所形成的空隙61c的寬度的長度為L1。第二組磁場板612所形成的空隙61d的寬度的長度為L2。第三組磁場板613所形成的空隙61e的寬度的長度為L3。磁場板611、磁場板612及磁場板613按該順序排列,且配置於靶保持器32的上表面部320。Specifically, the pair of magnetic field intensity adjustment plates 610 is a magnetic field plate group composed of a plurality of paired magnetic field plates. As shown in FIG. 12 , in this embodiment, a pair of magnetic field adjustment plates 610 has three pairs of magnetic field plates 611 , 612 and 613 in the length direction of the magnetic field adjustment plate 610 . The width and length of the gap 61c formed by the first group of magnetic field plates 611 is L1. The width and length of the gap 61d formed by the second group of magnetic field plates 612 is L2. The width and length of the gap 61e formed by the third group of magnetic field plates 613 is L3. The magnetic field plate 611 , the magnetic field plate 612 , and the magnetic field plate 613 are arranged in this order and arranged on the upper surface portion 320 of the target holder 32 .

於磁場板611、磁場板612及磁場板613,與磁場強度調整板61同樣地,形成有沿磁場強度調整板610的寬度方向延伸的長孔(於圖12中未圖示)。藉此,可規定空隙61c、空隙61d及空隙61e各自的寬度的長度L1、長度L2及長度L3。即,藉由分別調整長度L1、長度L2及長度L3,可根據靶30的長度方向上的位置來調整平行磁場的強度。由於可容易地降低靶30的長度方向上的平行磁場的強度的不均,因此特別是在靶30為長條狀的情況下可預料到大的效果。Like the magnetic field adjustment plate 61 , long holes (not shown in FIG. 12 ) extending in the width direction of the magnetic field adjustment plate 610 are formed in the magnetic field plate 611 , the magnetic field plate 612 , and the magnetic field plate 613 . Thereby, the length L1, the length L2, and the length L3 of the respective widths of the gap 61c, the gap 61d, and the gap 61e can be specified. That is, by adjusting the length L1, the length L2, and the length L3 respectively, the intensity of the parallel magnetic field can be adjusted according to the position of the target 30 in the longitudinal direction. Since the unevenness of the intensity of the parallel magnetic field in the longitudinal direction of the target 30 can be easily reduced, a large effect can be expected particularly when the target 30 is elongated.

此處,一般於靶30的長度方向上,越接近靶30的端部區域,平行磁場的強度越容易變弱。因此,例如,如圖12所示,使與靶30的兩端部區域對應的空隙的寬度61c及寬度61e較與靶30的中央區域對應的空隙61d的寬度窄(L1≒L3<L2),藉此,可使空隙61c及空隙61e中的磁場強度較空隙61d的磁場強度強。Here, in general, in the longitudinal direction of the target 30 , the closer to the end region of the target 30 , the weaker the intensity of the parallel magnetic field tends to be. Therefore, for example, as shown in FIG. 12 , the widths 61c and 61e of the gaps corresponding to the two end regions of the target 30 are made narrower than the width of the gap 61d corresponding to the central region of the target 30 (L1≒L3<L2), Thereby, the magnetic field strength in the gap 61c and the gap 61e can be made stronger than the magnetic field strength in the gap 61d.

但是,只要調整寬度61c、寬度61d及寬度61e,使得平行磁場的強度遍及靶30的整個表面地一致即可。例如,亦可根據靶30的配置等,將長度L1、長度L2及長度L3分別設為不同的長度。However, what is necessary is just to adjust width 61c, width 61d, and width 61e so that the intensity|strength of a parallel magnetic field may become uniform over the whole surface of the target 30. FIG. For example, the length L1, the length L2, and the length L3 may be set to different lengths depending on the arrangement of the target 30 or the like.

再者,磁場強度調整板610未必需要被分割為磁場板611、磁場板612及磁場板613此三個分區,可被分割為任意的數量。另外,藉由一對磁場強度調整板61分別彎曲,於磁場強度調整板61的長度方向上的各位置上,寬度61a的長度亦可不同。例如,亦可規定磁場強度調整板61的形狀,使得於磁場強度調整板61的長度方向的中央部上寬度61a成為最大。Furthermore, the magnetic field intensity adjustment plate 610 does not necessarily need to be divided into three partitions of the magnetic field plate 611 , the magnetic field plate 612 and the magnetic field plate 613 , and can be divided into any number. In addition, the length of the width 61 a may be different at each position in the longitudinal direction of the magnetic field intensity adjustment plate 61 by bending the pair of magnetic field intensity adjustment plates 61 respectively. For example, the shape of the magnetic field intensity adjustment plate 61 may be defined such that the width 61 a becomes the largest at the central portion in the longitudinal direction of the magnetic field intensity adjustment plate 61 .

另外,於本實施方式中,磁場強度調整板610兩者被分割為多個分區,但並不限於此。例如,亦可僅將其中一個磁場強度調整板610分割為多個分區。即便在此情況下,亦可各別地調整磁場強度調整板610的長度方向上的各位置的寬度。In addition, in this embodiment, both the magnetic field intensity adjustment plate 610 is divided into a plurality of partitions, but it is not limited thereto. For example, only one of the magnetic field intensity adjustment plates 610 may be divided into multiple partitions. Even in this case, the width of each position in the longitudinal direction of the magnetic field intensity adjustment plate 610 can be individually adjusted.

〔變形例1〕 於實施方式1中,作為具有與磁構件不同的磁導率的物質,於空隙61a中插入有空氣。於本變形例中,亦可將具有與空氣不同的磁導率的物質插入至空隙61a。藉此,可調整磁路的磁阻,其結果,可調整平行磁場的強度。例如,在將磁導率為空氣磁導率(1.26×10 -6μH/m)的約100倍的碳鋼(磁導率:1.26×10 -4μH/m)插入至空隙61a的情況下,磁路的磁阻為1/100。因此,可提高平行磁場的強度。此外,亦可於空隙61a中插入非磁性金屬(例:鋁)或工程塑膠(例:聚醚醚酮(Poly Ether Ether Ketone,PEEK))等磁導率較磁構件低的物質。 [Modification 1] In Embodiment 1, air is inserted into the gap 61a as a substance having a magnetic permeability different from that of the magnetic member. In this modified example, a substance having a magnetic permeability different from that of air may be inserted into the gap 61a. Thereby, the reluctance of the magnetic circuit can be adjusted, and as a result, the strength of the parallel magnetic field can be adjusted. For example, in the case of inserting carbon steel (permeability: 1.26×10 −4 μH/m) about 100 times that of air (permeability: 1.26×10 −4 μH/m) into the gap 61 a , the reluctance of the magnetic circuit is 1/100. Therefore, the strength of the parallel magnetic field can be increased. In addition, non-magnetic metals (for example: aluminum) or engineering plastics (for example: Poly Ether Ether Ketone (PEEK)) and other substances with lower magnetic permeability than the magnetic components can also be inserted into the gap 61 a.

另外,磁場強度調整板61亦可並非由一對磁構件構成,而是由不具有空隙的一張板(例如,包含PEEK的板)構成。在此情況下,藉由將磁場強度調整板61更換為具有與該磁場強度調整板61的磁導率不同的磁導率的其他磁場強度調整板61,可變更磁路的磁阻。In addition, the magnetic field strength adjustment plate 61 may be formed not from a pair of magnetic members but from a single plate (for example, a plate made of PEEK) without a gap. In this case, the magnetic resistance of the magnetic circuit can be changed by replacing the magnetic field strength adjustment plate 61 with another magnetic field strength adjustment plate 61 having a magnetic permeability different from that of the magnetic field strength adjustment plate 61 .

〔變形例2〕 於實施方式1中,於上表面部3的內部設置有一對磁鐵65,但設置磁鐵65的位置並不限定於該位置。例如,亦可於上表面部3的表面配置具有N極及S極的一個磁鐵來代替磁場強度調整板61。或者,亦可於上表面部3的表面配置N極的磁鐵及S極的磁鐵。在此情況下,可藉由更換磁鐵來調整平行磁場的強度。 [Modification 2] In Embodiment 1, the pair of magnets 65 is provided inside the upper surface part 3, but the position where the magnets 65 are provided is not limited to this position. For example, instead of the magnetic field intensity adjustment plate 61 , one magnet having an N pole and an S pole may be disposed on the surface of the upper surface portion 3 . Alternatively, an N-pole magnet and an S-pole magnet may be arranged on the surface of the upper surface portion 3 . In this case, the strength of the parallel magnetic field can be adjusted by replacing the magnet.

〔變形例3〕 於以上所述的實施方式中,藉由天線20所產生的電漿22進行了離子化,但並不限定於此。例如,亦可無天線20,而藉由磁路形成產生磁控管放電的強度以上的平行磁場。 [Modification 3] In the above-mentioned embodiments, the plasma 22 generated by the antenna 20 is ionized, but the present invention is not limited thereto. For example, without the antenna 20, a magnetic circuit may form a parallel magnetic field having a strength equal to or greater than that of a magnetron discharge.

〔總結〕 本發明的一形態的濺鍍裝置於真空容器內對靶進行濺鍍而於基板上成膜,且所述濺鍍裝置中,所述真空容器包括保持所述靶的至少一個保持部,所述保持部包括:氣體導入部,向所述保持部導入氣體;以及一對開口部,於自鉛垂下方向觀察於所述保持部中配置所述靶的靶配置位置時,遍及所述靶配置位置的周圍的至少一部分且設置於隔著所述靶配置位置相向的位置,將導入至所述保持部內的所述氣體放出至所述真空容器內。 〔Summarize〕 A sputtering device according to one aspect of the present invention sputters a target in a vacuum container to form a film on a substrate, and in the sputtering device, the vacuum container includes at least one holding portion for holding the target, and the sputtering device includes: The holding unit includes: a gas introduction unit for introducing gas into the holding unit; and a pair of openings extending over the target placement position where the target is placed in the holding unit when viewed from a vertically downward direction. At least a part of its periphery is provided at a position opposite to the target arrangement position, and the gas introduced into the holding part is released into the vacuum container.

根據所述結構,能夠以大致均勻的壓力自靶的周圍遍及靶的整個表面地供給氣體。因此,可減少靶的整個表面上的氣體分佈的不均。因此,可降低於基板上成膜的薄膜的膜厚發生偏差的可能性。According to the above structure, the gas can be supplied at a substantially uniform pressure from the periphery of the target over the entire surface of the target. Therefore, unevenness in gas distribution over the entire surface of the target can be reduced. Therefore, the possibility of variations in the film thickness of the thin film formed on the substrate can be reduced.

於本發明的一形態的濺鍍裝置中,亦可為:自所述鉛垂下方向觀察時的所述靶配置位置的形狀為矩形形狀,所述開口部是遍及所述靶配置位置的相向的邊的整體而設置。In the sputtering apparatus according to one aspect of the present invention, the shape of the target arrangement position when viewed from the vertically downward direction may be a rectangular shape, and the openings may face each other across the target arrangement position. set for the whole of the edge.

根據所述結構,可遍及靶的整個表面更均勻地供給氣體。According to the structure, the gas can be supplied more uniformly over the entire surface of the target.

於本發明的一形態的濺鍍裝置中,所述開口部亦可遍及所述靶配置位置的相向的長邊的整體而設置。In the sputtering apparatus of one aspect of this invention, the said opening part may be provided over the whole of the long side which opposes the said target arrangement position.

根據所述結構,可遍及靶的整個表面更均勻地供給氣體。According to the structure, the gas can be supplied more uniformly over the entire surface of the target.

於本發明的一形態的濺鍍裝置中,亦可為:所述保持部包括磁鐵以及被磁鐵磁化的磁構件,所述磁鐵及所述磁構件形成磁路,所述磁路於所述靶配置位置上形成磁場,於所述磁路的一部分形成空隙,形成有所述空隙的所述磁路的一部分設置於所述真空容器的外部。In the sputtering apparatus according to one aspect of the present invention, the holding unit may include a magnet and a magnetic member magnetized by the magnet, the magnet and the magnetic member form a magnetic circuit, and the magnetic circuit is connected to the target. A magnetic field is formed at an arrangement position, a gap is formed in a part of the magnetic circuit, and a part of the magnetic circuit in which the gap is formed is provided outside the vacuum container.

根據所述結構,藉由設置於真空容器的外部的空隙,可在不將真空容器打開的情況下調整磁路的磁阻。According to the above structure, the magnetic resistance of the magnetic circuit can be adjusted without opening the vacuum container by the gap provided outside the vacuum container.

於本發明的一形態的濺鍍裝置中,所述保持部亦可包括對所述空隙的寬度進行調整的調整機構。In the sputtering device according to one aspect of the present invention, the holding unit may include an adjustment mechanism for adjusting the width of the gap.

根據所述結構,藉由調整空隙的寬度,可調整磁路的磁阻。According to the above structure, by adjusting the width of the air gap, the reluctance of the magnetic circuit can be adjusted.

於本發明的一形態的濺鍍裝置中,亦可為:所述調整機構包括一對磁調整構件,所述一對磁調整構件作為所述磁構件的一部分而設置於所述保持部的上表面部,並規定所述空隙,於所述一對磁調整構件中的至少一個磁調整構件形成有長孔,所述長孔貫通作為所述磁構件的一部分而將所述磁調整構件固定於所述保持部的固定構件,且沿所述空隙的寬度方向延伸,所述長孔中的所述固定構件的貫通位置能夠改變。In the sputtering apparatus according to one aspect of the present invention, the adjustment mechanism may include a pair of magnetic adjustment members, and the pair of magnetic adjustment members may be provided on the holding portion as a part of the magnetic member. surface portion, and define the gap, and at least one magnetic adjustment member of the pair of magnetic adjustment members is formed with a long hole, and the long hole passes through as a part of the magnetic member to fix the magnetic adjustment member to the The fixing member of the holding part extends along the width direction of the gap, and the penetration position of the fixing member in the long hole can be changed.

根據所述結構,藉由使磁調整構件中的長孔的貫通位置能夠改變,可變更空隙的寬度。According to the above configuration, the width of the gap can be changed by allowing the penetrating position of the long hole in the magnetic adjustment member to be changed.

於本發明的一形態的濺鍍裝置中,亦可為:自所述鉛垂下方向觀察時的所述靶配置位置的形狀為矩形形狀,所述一對磁調整構件是沿所述靶配置位置的長度方向延伸而設置,所述一對磁調整構件中的至少一個磁調整構件沿著所述長度方向被分割為多個分區,藉由針對所述多個分區的每一個規定所述長孔中的所述固定構件的貫通位置,來規定所述空隙的寬度。In the sputtering apparatus according to one aspect of the present invention, the shape of the target arrangement position when viewed from the vertically downward direction may be a rectangular shape, and the pair of magnetic adjustment members may be arranged along the target arrangement position. The length direction of the pair of magnetic adjustment members is extended, and at least one magnetic adjustment member in the pair of magnetic adjustment members is divided into a plurality of partitions along the length direction, and the elongated hole is defined for each of the plurality of partitions. The width of the gap is defined by the penetration position of the fixing member.

根據所述結構,可針對每個分區規定不同的空隙的寬度。因此,可於靶配置位置的長度方向上調整磁路的磁阻。According to the structure, different widths of the gaps can be specified for each partition. Therefore, the magnetic resistance of the magnetic circuit can be adjusted in the longitudinal direction of the target arrangement position.

於本發明的一形態的濺鍍裝置中,於所述空隙中亦可插入具有與所述磁構件不同的磁導率的物質。In the sputtering apparatus according to one aspect of the present invention, a substance having a magnetic permeability different from that of the magnetic member may be inserted into the gap.

根據所述結構,藉由在空隙中插入磁導率與磁構件不同的物質,可調整磁路的磁阻。According to the above structure, the magnetic resistance of the magnetic circuit can be adjusted by inserting a substance having a magnetic permeability different from that of the magnetic member in the gap.

於本發明的一形態的濺鍍裝置中,亦可包括多個所述保持部。In the sputtering apparatus which concerns on 1 aspect of this invention, the said holding|maintenance part may be provided in some numbers.

根據所述結構,可藉由多個靶對更大的基板進行濺鍍。According to the structure, a larger substrate can be sputtered with a plurality of targets.

於本發明的一形態的濺鍍裝置中,亦可為:所述真空容器包括對所述真空容器的內部進行真空排氣的多個排氣部,所述排氣部與所述保持部鄰接地設置。In the sputtering apparatus according to one aspect of the present invention, the vacuum container may include a plurality of exhaust parts for evacuating the inside of the vacuum container, and the exhaust parts may be adjacent to the holding part. ground setting.

根據所述結構,可使靶的整個表面上的氣體的分佈更均勻化。According to the structure, the distribution of the gas over the entire surface of the target can be made more uniform.

於本發明的一形態的濺鍍裝置中,亦可為:所述保持部包括將所述氣體導入部與所述開口部連通的氣體路徑,所述氣體路徑包括:主路徑,接受自所述氣體導入部導入的氣體;以及多個分支路徑,與所述主路徑連通,將所述主路徑內的氣體導入至所述開口部,所述多個分支路徑各自的粗細較所述主路徑的粗細小。In the sputtering device according to one aspect of the present invention, the holding part may include a gas path connecting the gas introduction part and the opening part, and the gas path may include a main path received from the the gas introduced by the gas introduction part; and a plurality of branch paths communicating with the main path to introduce the gas in the main path to the opening, the thickness of each of the plurality of branch paths being smaller than that of the main path thick and small.

根據所述結構,可提高經由分支路徑自開口部放出的氣體的流速,因此能夠以於靶的整個表面上疏密的部分變少的方式將氣體分散。According to the above configuration, the flow velocity of the gas discharged from the opening through the branch path can be increased, so that the gas can be dispersed so that the dense and dense parts on the entire surface of the target are reduced.

〔附記事項〕 本發明並不限定於以上所述的各實施方式,能夠於申請專利範圍所示的範圍內進行各種變更,將不同的實施方式中分別揭示的技術手段適宜組合而得的實施方式亦包含於本發明的技術範圍內。 [Additional notes] The present invention is not limited to the above-mentioned embodiments, and various changes can be made within the range indicated in the patent claims. Embodiments obtained by appropriately combining the technical means disclosed in different embodiments are also included in this document. within the technical scope of the invention.

1:濺鍍裝置 2:真空容器 3、320:上表面部 4:真空排氣裝置 6:氣體源 8:流量調節器 10:氣體 12:基板 14:基板保持器 16:基板偏置電源 20:天線 22:電漿 24:高頻電源 26:整合電路 30:靶 30a:靶配置位置 32:靶保持器(保持部) 34:靶偏置電源 40、41、43:絕緣部 46:控制裝置 50:氣體導入配管 51:氣體導入部 52:氣體路徑(主路徑) 53:氣體分支路徑(氣體路徑、分支路徑) 54:氣體放出口(開口部) 55:排氣口(排氣部) 61、610:磁場強度調整板(磁調整構件) 61a、61c、61d、61e:空隙 61b:長孔 62:磁路徑螺栓(固定構件) 63:第一磁性板(磁構件) 64:磁鐵保持部 65:磁鐵 66:第二磁性板(磁構件) 67:第三磁性板(磁構件) 71:電極 72:陽極 81:冷卻水口 82:冷卻水路徑 321:靶主體 322:背板 421:絕緣襯套 422:第一絕緣板 423:第二絕緣板 501:氣體絕緣配管 521:氣體路徑蓋 522:節流孔 611、612、613:磁場板(磁調整構件) 1201、1202:符號 L、L1、L2、L3:長度 Pr:高頻電力 Vs:基板偏置電壓 Vt:靶偏置電壓 1: Sputtering device 2: Vacuum container 3. 320: upper surface 4: Vacuum exhaust device 6: Gas source 8: Flow regulator 10: gas 12: Substrate 14: Substrate holder 16: Substrate bias power supply 20: Antenna 22: Plasma 24: High frequency power supply 26: integrated circuit 30: target 30a: target configuration position 32: Target holder (holding part) 34: Target bias power supply 40, 41, 43: insulation part 46: Control device 50: Gas introduction piping 51: Gas introduction part 52: Gas path (main path) 53: Gas branch path (gas path, branch path) 54: Gas outlet (opening) 55: Exhaust port (exhaust part) 61, 610: Magnetic field strength adjustment plate (magnetic adjustment member) 61a, 61c, 61d, 61e: gaps 61b: long hole 62: Magnetic path bolt (fixed member) 63: The first magnetic plate (magnetic member) 64:Magnet holder 65: magnet 66: Second magnetic plate (magnetic component) 67: The third magnetic plate (magnetic component) 71: electrode 72: anode 81: cooling water port 82: Cooling water path 321: target subject 322: Backplane 421: insulating bushing 422: The first insulation board 423: Second insulation board 501: Gas insulated piping 521: Gas path cover 522: Orifice 611, 612, 613: magnetic field plate (magnetic adjustment member) 1201, 1202: symbols L, L1, L2, L3: Length Pr: high frequency power Vs: Substrate bias voltage Vt: target bias voltage

圖1是表示實施方式1的濺鍍裝置的整體結構例的圖。 圖2是實施方式1的靶保持器的圖1中的A-A向視圖,且是組裝了靶保持器的狀態下的俯視圖。 圖3是實施方式1的靶保持器的圖1中的B-B向視圖,且是組裝了靶保持器的狀態下的仰視圖。 圖4是實施方式1的靶保持器的圖1中的C-C向視圖。 圖5是實施方式1的靶保持器的圖1中的D-D向視圖。 圖6是實施方式1的靶保持器的圖1中的E-E向視圖。 圖7是實施方式1的靶保持器的圖2中的F-F剖面圖。 圖8是實施方式1的靶保持器的圖2中的G-G剖面圖。 圖9是圖2中的H部的放大圖。 圖10是表示實施方式2的真空容器內的詳細結構的剖面圖。 圖11是實施方式2的靶保持器的圖10中的I-I向視圖,且是組裝了靶保持器的狀態下的仰視圖。 圖12是實施方式1及實施方式3的磁場強度調整板的概略圖。 FIG. 1 is a diagram showing an example of the overall configuration of a sputtering apparatus according to Embodiment 1. FIG. 2 is a view taken along the line A-A in FIG. 1 of the target holder according to Embodiment 1, and is a plan view in a state where the target holder is assembled. 3 is a view taken along the line B-B in FIG. 1 of the target holder according to Embodiment 1, and is a bottom view in a state where the target holder is assembled. FIG. 4 is a view taken along the line C-C in FIG. 1 of the target holder according to Embodiment 1. FIG. 5 is a D-D arrow view in FIG. 1 of the target holder according to Embodiment 1. FIG. FIG. 6 is a view taken along the line E-E in FIG. 1 of the target holder according to Embodiment 1. FIG. 7 is a cross-sectional view of the target holder according to Embodiment 1 taken along line F-F in FIG. 2 . FIG. 8 is a G-G cross-sectional view of the target holder in FIG. 2 according to Embodiment 1. FIG. FIG. 9 is an enlarged view of part H in FIG. 2 . 10 is a cross-sectional view showing a detailed structure inside a vacuum vessel according to Embodiment 2. FIG. Fig. 11 is a view taken along the line I-I in Fig. 10 of the target holder according to Embodiment 2, and is a bottom view of the state where the target holder is assembled. FIG. 12 is a schematic diagram of a magnetic field intensity adjustment plate according to Embodiments 1 and 3. FIG.

1:濺鍍裝置 1: Sputtering device

2:真空容器 2: Vacuum container

3、320:上表面部 3. 320: upper surface

4:真空排氣裝置 4: Vacuum exhaust device

6:氣體源 6: Gas source

8:流量調節器 8: Flow regulator

10:氣體 10: gas

12:基板 12: Substrate

14:基板保持器 14: Substrate holder

16:基板偏置電源 16: Substrate bias power supply

20:天線 20: Antenna

22:電漿 22: Plasma

24:高頻電源 24: High frequency power supply

26:整合電路 26: integrated circuit

30:靶 30: target

32:靶保持器(保持部) 32: Target holder (holding part)

34:靶偏置電源 34: Target bias power supply

40、41、43:絕緣部 40, 41, 43: insulation part

46:控制裝置 46: Control device

50:氣體導入配管 50: Gas introduction piping

51:氣體導入部 51: Gas introduction part

501:氣體絕緣配管 501: Gas insulated piping

Pr:高頻電力 Pr: high frequency power

Vs:基板偏置電壓 Vs: Substrate bias voltage

Vt:靶偏置電壓 Vt: target bias voltage

Claims (11)

一種濺鍍裝置,於真空容器內對靶進行濺鍍而於基板上成膜,且所述濺鍍裝置中, 所述真空容器包括保持所述靶的至少一個保持部, 所述保持部包括: 氣體導入部,向所述保持部導入氣體;以及 一對開口部,於自鉛垂下方向觀察於所述保持部中配置所述靶的靶配置位置時,遍及所述靶配置位置的周圍的至少一部分且設置於隔著所述靶配置位置相向的位置,將導入至所述保持部內的所述氣體放出至所述真空容器內。 A sputtering device for sputtering a target in a vacuum container to form a film on a substrate, and in the sputtering device, the vacuum container includes at least one holding portion holding the target, The holding part includes: a gas introduction part for introducing gas into the holding part; and A pair of openings are provided at positions facing each other across at least a part of the periphery of the target placement position when the target placement position where the target is placed in the holding portion is viewed from a vertically downward direction. position, and release the gas introduced into the holding part into the vacuum container. 如請求項1所述的濺鍍裝置,其中, 自所述鉛垂下方向觀察時的所述靶配置位置的形狀為矩形形狀, 所述開口部是遍及所述靶配置位置的相向的邊的整體而設置。 The sputtering device as claimed in item 1, wherein, The shape of the target arrangement position when viewed from the vertically downward direction is a rectangular shape, The opening is provided over the entirety of opposing sides of the target arrangement position. 如請求項1或請求項2所述的濺鍍裝置,其中, 所述開口部是遍及所述靶配置位置的相向的長邊的整體而設置。 The sputtering device as claimed in claim 1 or claim 2, wherein, The opening is provided over the entire length of the opposing long sides of the target arrangement position. 如請求項1至請求項3中任一項所述的濺鍍裝置,其中, 所述保持部包括磁鐵以及被磁鐵磁化的磁構件, 所述磁鐵及所述磁構件形成磁路,所述磁路於所述靶配置位置上形成磁場, 於所述磁路的一部分形成空隙, 形成有所述空隙的所述磁路的一部分設置於所述真空容器的外部。 The sputtering device according to any one of claim 1 to claim 3, wherein, The holding part includes a magnet and a magnetic member magnetized by the magnet, The magnet and the magnetic member form a magnetic circuit, and the magnetic circuit forms a magnetic field at the position where the target is arranged, forming a gap in part of the magnetic circuit, A part of the magnetic circuit in which the gap is formed is provided outside the vacuum container. 如請求項4所述的濺鍍裝置,其中,所述保持部包括對所述空隙的寬度進行調整的調整機構。The sputtering device according to claim 4, wherein the holding part includes an adjustment mechanism for adjusting the width of the gap. 如請求項5所述的濺鍍裝置,其中, 所述調整機構包括一對磁調整構件,所述一對磁調整構件作為所述磁構件的一部分而設置於所述保持部的上表面部,並規定所述空隙, 於所述一對磁調整構件中的至少一個磁調整構件形成有長孔,所述長孔貫通作為所述磁構件的一部分而將所述磁調整構件固定於所述保持部的固定構件,且沿所述空隙的寬度方向延伸, 所述長孔中的所述固定構件的貫通位置能夠改變。 The sputtering device as claimed in item 5, wherein, The adjustment mechanism includes a pair of magnetic adjustment members provided as a part of the magnetic member on an upper surface portion of the holding portion and defining the gap, At least one magnetic adjustment member of the pair of magnetic adjustment members is formed with a long hole penetrating through a fixing member that is a part of the magnetic member and fixes the magnetic adjustment member to the holding portion, and extending along the width direction of the void, The penetration position of the fixing member in the long hole can be changed. 如請求項6所述的濺鍍裝置,其中, 自所述鉛垂下方向觀察時的所述靶配置位置的形狀為矩形形狀, 所述一對磁調整構件是沿所述靶配置位置的長度方向延伸而設置, 所述一對磁調整構件中的至少一個磁調整構件沿著所述長度方向被分割為多個分區, 藉由針對所述多個分區的每一個規定所述長孔中的所述固定構件的貫通位置,來規定所述空隙的寬度。 The sputtering device as claimed in claim 6, wherein, The shape of the target arrangement position when viewed from the vertically downward direction is a rectangular shape, The pair of magnetic adjustment members are provided extending along the length direction of the target arrangement position, At least one magnetic adjustment member of the pair of magnetic adjustment members is divided into a plurality of partitions along the length direction, The width of the gap is specified by specifying the penetration position of the fixing member in the elongated hole for each of the plurality of partitions. 如請求項4至請求項7中任一項所述的濺鍍裝置,其中,於所述空隙中插入具有與所述磁構件不同的磁導率的物質。The sputtering apparatus according to any one of claim 4 to claim 7, wherein a substance having a magnetic permeability different from that of the magnetic member is inserted into the gap. 如請求項1至請求項8中任一項所述的濺鍍裝置,包括多個所述保持部。The sputtering device according to any one of claim 1 to claim 8, comprising a plurality of holding parts. 如請求項1至請求項9中任一項所述的濺鍍裝置,其中,所述真空容器包括對所述真空容器的內部進行真空排氣的至少一個排氣部, 所述排氣部與所述保持部鄰接地設置。 The sputtering device according to any one of claim 1 to claim 9, wherein the vacuum container includes at least one exhaust part for vacuum exhausting the inside of the vacuum container, The exhaust portion is provided adjacent to the holding portion. 如請求項1至請求項10中任一項所述的濺鍍裝置,其中, 所述保持部包括將所述氣體導入部與所述開口部連通的氣體路徑, 所述氣體路徑包括: 主路徑,接受自所述氣體導入部導入的氣體;以及 多個分支路徑,與所述主路徑連通,將所述主路徑內的氣體導入至所述開口部, 所述多個分支路徑各自的粗細較所述主路徑的粗細小。 The sputtering device according to any one of claim 1 to claim 10, wherein, The holding portion includes a gas path that communicates the gas introduction portion with the opening portion, The gas path includes: a main path for receiving the gas introduced from the gas introduction part; and a plurality of branch paths communicated with the main path, leading the gas in the main path to the opening, A thickness of each of the plurality of branch paths is smaller than a thickness of the main path.
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