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TW201437407A - Film formation method for aluminum oxide and sputtering device - Google Patents

Film formation method for aluminum oxide and sputtering device Download PDF

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TW201437407A
TW201437407A TW102145671A TW102145671A TW201437407A TW 201437407 A TW201437407 A TW 201437407A TW 102145671 A TW102145671 A TW 102145671A TW 102145671 A TW102145671 A TW 102145671A TW 201437407 A TW201437407 A TW 201437407A
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sputtering
plasma
target
voltage
reactive gas
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TWI504773B (en
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Kazuto Ozaki
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Dainippon Screen Mfg
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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
    • C23C14/06Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the coating material
    • C23C14/08Oxides
    • C23C14/081Oxides of aluminium, magnesium or beryllium
    • 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
    • C23C14/0021Reactive sputtering or evaporation
    • C23C14/0036Reactive sputtering
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
    • C23C14/3492Variation of parameters during sputtering
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
    • C23C14/35Sputtering by application of a magnetic field, e.g. magnetron sputtering
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50Manufacturing or production processes characterised by the final manufactured product

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

Abstract

This invention enables formation of an aluminum oxide film by sputtering with the stable oxidation degree and the higher film formation rate. The film formation method for the aluminum oxide of this invention comprises the following steps: a first plasma generation step for generating plasma in a vacuum container introduced with the sputtering gas and the reactive gas; a second plasma generation step for imposing the sputtering voltage on the aluminum target to generate the magnetron plasma by the magnetostatic field; and a control step for controlling the amount of reactive gas introduced into the vacuum container. In addition, in the second plasma generation step, the sputtering voltage is subject to voltage control; in the control step, by means of making the sputtering current value reach the target current value, the amount of reactive gas introduced in the second plasma generation step is controlled; the first plasma generation step uses a high frequency antenna with winding less than one loop, and the high frequency inductance-coupled plasma is generated in the second plasma generation step.

Description

氧化鋁之成膜方法及濺鍍裝置 Alumina film forming method and sputtering device

本發明係關於一種用於太陽電池矽基板之鈍化膜之氧化鋁之利用反應性濺鍍之成膜技術。 The present invention relates to a film forming technique for utilizing reactive sputtering of alumina for a passivation film of a solar cell tantalum substrate.

近年來,伴隨著尋求太陽電池之高效化,亦在尋求p型矽表面之有效之鈍化膜。而且,關於矽晶圓p型面,具有正電荷之SiNx於場效上不能稱為適當,較理想為尋求一種具有負電荷之膜。 In recent years, along with the search for efficiency of solar cells, effective passivation films for p-type germanium surfaces have been sought. Moreover, regarding the p-type surface of the germanium wafer, the positive charge SiNx cannot be said to be suitable in field effect, and it is desirable to seek a film having a negative charge.

已知作為具有該負電荷之鈍化膜,以氧化鋁(Al2O3)為佳。而且,先前為了將氧化鋁用作鈍化膜,一直採用ALD(Atomic Layer Deposition,原子層沈積)法及PE-CVD(Plasma Enhanced Chemical Vapor Deposition,電漿增強化學氣體沈積)法。然而,ALD法成膜速度極慢、生產性較差,故而存在不適於量產之問題。又,PE-CVD法中使用所謂TMD(三甲基鋁)液之易燃性液體,故而存在需要密切注意裝置設計及原料之處理之問題。 It is known that as the passivation film having the negative charge, alumina (Al 2 O 3 ) is preferred. Further, in order to use alumina as a passivation film, an ALD (Atomic Layer Deposition) method and a PE-CVD (Plasma Enhanced Chemical Vapor Deposition) method have been used. However, the film formation speed of the ALD method is extremely slow and the productivity is poor, so there is a problem that it is not suitable for mass production. Further, since the flammable liquid of the so-called TMD (trimethylaluminum) liquid is used in the PE-CVD method, there is a problem that it is necessary to pay close attention to the design of the device and the treatment of the raw material.

另一方面,亦正在研究利用磁控濺鍍法之氧化鋁膜之成膜。磁控濺鍍法作為薄膜形成方法之一而廣泛應用於半導體、液晶顯示裝置、磁性記錄裝置、光學薄膜等製造領域中。於磁控濺鍍法中有高頻磁控濺鍍法(專利文獻1)或反應性DC(Direct Current,直流)磁控濺鍍法(專利文獻2)等,該高頻磁控濺鍍法係使用氧化物、氮化物、氟化 物等化合物靶材,藉由將高頻電源用作濺鍍電源而形成化合物之薄膜,該反應性DC磁控濺鍍法係使用金屬靶材,將直流電源用作濺鍍電源,並且導入反應性氣體,從而形成金屬之氧化物、氮化物、氟化物等之薄膜,無論哪種方法均係根據用途而被廣泛使用。 On the other hand, the formation of an aluminum oxide film by magnetron sputtering is also being studied. The magnetron sputtering method is widely used in the manufacturing fields of semiconductors, liquid crystal display devices, magnetic recording devices, optical films, and the like as one of film forming methods. In the magnetron sputtering method, there are a high frequency magnetron sputtering method (Patent Document 1) or a reactive DC (Direct Current) magnetron sputtering method (Patent Document 2), etc., the high frequency magnetron sputtering method. Use oxides, nitrides, fluorination A compound target such as a compound, which forms a film of a compound by using a high-frequency power source as a sputtering power source, which uses a metal target, uses a DC power source as a sputtering power source, and introduces a reaction. A gas is formed into a film of a metal oxide, a nitride, a fluoride or the like, and any method is widely used depending on the use.

[先前技術文獻] [Previous Technical Literature] [專利文獻] [Patent Literature]

[專利文獻1]日本專利特開2004-31493號公報 [Patent Document 1] Japanese Patent Laid-Open Publication No. 2004-31493

[專利文獻2]日本專利特開平8-232064號公報 [Patent Document 2] Japanese Patent Laid-Open No. Hei 8-232064

然而,由於氧化鋁之硬度非常高、或靶材表面由鋁之氧化物覆蓋,故而即便採用專利文獻1、2之方法,亦存在難以提昇成膜速度之問題。又,為了於濺鍍法中於p型Si表面形成鈍化效果較佳之氧化鋁膜,必須以較高精度將所要成膜之氧化鋁之氧化度控制為固定。然而,於藉由專利文獻1、2之方法成膜氧化鋁膜之情形時,通常係進行以電力固定模式驅動濺鍍電源之控制(濺鍍電壓之定電力控制),因而氧化鋁之氧化度因躍遷模式之成膜而變得不穩定。因此,亦存在鋁過度氧化、或氧化變得不充分之情況交替重複,而使所要成膜之氧化鋁之氧化度不穩定等問題。 However, since the hardness of alumina is very high, or the surface of the target is covered with an oxide of aluminum, even if the methods of Patent Documents 1 and 2 are employed, there is a problem that it is difficult to increase the film formation speed. Further, in order to form an aluminum oxide film having a good passivation effect on the surface of the p-type Si in the sputtering method, it is necessary to control the degree of oxidation of the aluminum oxide to be formed into a film with high precision. However, in the case where the aluminum oxide film is formed by the methods of Patent Documents 1 and 2, the control of driving the sputtering power source in the electric power fixed mode (the power control of the sputtering voltage) is usually performed, and thus the oxidation degree of the aluminum oxide is performed. It becomes unstable due to film formation in the transition mode. Therefore, there is also a problem that the aluminum is excessively oxidized or the oxidation is insufficient, and the degree of oxidation of the alumina to be film-formed is unstable.

本發明係為解決此種問題而完成者,其目的在於提供一種於反應性濺鍍中能夠使氧化度穩定地、且以較快之成膜速度成膜氧化鋁之技術。 The present invention has been made to solve such a problem, and an object of the present invention is to provide a technique for forming alumina on a film formation rate at a film formation rate which is stable in oxidation degree in reactive sputtering.

為解決上述問題,第1態樣之氧化鋁之成膜方法係於設置有形成靜磁場之磁控陰極之真空容器中,將濺鍍氣體及氧氣之反應性氣體以該真空容器內之壓力達到目標壓力之方式進行控制並導入,對設置於 該陰極之鋁靶進行濺鍍,於與該鋁靶對向之矽基板上形成氧化膜;且包括以下步驟:第1電漿產生步驟,其係於導入有上述濺鍍氣體及上述反應性氣體之真空容器內產生電漿;第2電漿產生步驟,其係對上述鋁靶施加負電壓、包含負電壓與正電壓之直流脈衝、或交流之任一種濺鍍電壓,藉由上述靜磁場而產生磁控電漿;及控制步驟,其控制導入至上述真空容器內之上述反應性氣體之導入量;上述第2電漿產生步驟係將上述濺鍍電壓進行定電壓控制之步驟;上述控制步驟係如下步驟,即,以流動於上述磁控陰極之濺鍍電流值達到目標電流值之方式,控制上述第2電漿產生步驟中上述反應性氣體之導入量;上述第1電漿產生步驟係如下步驟,即,使用設置於上述真空容器內且包含卷數未達一圈之導體之高頻天線,至少於上述第2電漿產生步驟中產生高頻電感耦合電漿。 In order to solve the above problems, the film forming method of the first aspect is formed in a vacuum vessel provided with a magnetron cathode for forming a static magnetic field, and the reactive gas of the sputtering gas and the oxygen gas is reached by the pressure in the vacuum vessel. The target pressure is controlled and imported, and is set to The aluminum target of the cathode is sputtered to form an oxide film on the substrate opposite to the aluminum target; and the method includes the following steps: a first plasma generating step of introducing the sputtering gas and the reactive gas a plasma is generated in the vacuum vessel; a second plasma generating step is to apply a negative voltage, a DC pulse including a negative voltage and a positive voltage, or a sputtering voltage to the aluminum target, by the static magnetic field. Generating a magnetron plasma; and controlling a step of controlling an introduction amount of the reactive gas introduced into the vacuum vessel; and the second plasma generating step is a step of controlling a voltage of the sputtering voltage; the control step a step of controlling the introduction amount of the reactive gas in the second plasma generating step such that the sputtering current value flowing through the magnetron cathode reaches a target current value; the first plasma generating step is a high frequency inductive coupling generated in at least the second plasma generating step by using a high frequency antenna disposed in the vacuum container and including a conductor having a number of windings less than one turn Plasma.

第2態樣之氧化鋁之成膜方法係如第1態樣之氧化鋁之成膜方法,其中上述目標電流值係所要成膜之氧化鋁之氧化度成為如下氧化度時之上述濺鍍電流值,即化學計量之氧化鋁與氧化度較化學計量之氧化鋁低之氧化鋁各自之氧化度之邊界附近的氧化度。 The film forming method of the second aspect is the film forming method of the aluminum oxide according to the first aspect, wherein the target current value is the sputtering current when the degree of oxidation of the aluminum oxide to be film-formed becomes the following oxidation degree. The value is the degree of oxidation near the boundary between the stoichiometric amount of alumina and the degree of oxidation of each of the alumina having a lower oxidation degree than the stoichiometric amount of alumina.

第3態樣之氧化鋁之成膜方法係如第1或第2態樣之氧化鋁之成膜方法,其中上述控制步驟係如下步驟,即,根據上述反應性氣體之電漿發光強度之變化而預測上述濺鍍電流值之變化,以上述濺鍍電流值達到上述目標電流值之方式,控制上述反應性氣體之導入量。 The film forming method of the third aspect of the alumina is a film forming method of the first or second aspect, wherein the controlling step is a step of changing the luminous intensity of the plasma according to the reactive gas. The change in the sputtering current value is predicted, and the introduction amount of the reactive gas is controlled such that the sputtering current value reaches the target current value.

第4態樣之氧化鋁之成膜方法係如第1或第2態樣之氧化鋁之成膜方法,其中上述濺鍍電壓為負電壓。 The film forming method of the aluminum oxide according to the fourth aspect is a film forming method of alumina according to the first or second aspect, wherein the sputtering voltage is a negative voltage.

第5態樣之氧化鋁之成膜方法係如第1或第2態樣之氧化鋁之成膜方法,其中上述目標壓力為0.2Pa以上且7Pa以下。 The film forming method of the aluminum according to the fifth aspect is a film forming method of alumina according to the first or second aspect, wherein the target pressure is 0.2 Pa or more and 7 Pa or less.

第6態樣之氧化鋁之成膜方法係如第5態樣之氧化鋁之成膜方法,其中上述目標壓力為0.4Pa以上且2Pa以下。 The film forming method of the sixth aspect is a film forming method of the aluminum according to the fifth aspect, wherein the target pressure is 0.4 Pa or more and 2 Pa or less.

第7態樣之氧化鋁之成膜方法係如第1或第2態樣之氧化鋁之成膜方法,其中上述濺鍍電壓之負電壓之絕對值為100V以上且300V以下。 The film forming method of the aluminum oxide according to the seventh aspect is the film forming method of the first or second aspect, wherein the absolute value of the negative voltage of the sputtering voltage is 100 V or more and 300 V or less.

第8態樣之氧化鋁之成膜方法係如第7態樣之氧化鋁之成膜方法,其中上述濺鍍電壓之負電壓之絕對值為150V以上且250V以下。 The film forming method of the aluminum oxide according to the eighth aspect is the film forming method of the aluminum oxide according to the seventh aspect, wherein the absolute value of the negative voltage of the sputtering voltage is 150 V or more and 250 V or less.

第9態樣之濺鍍裝置係於設置有形成靜磁場之磁控陰極之真空容器中,將濺鍍氣體及氧氣之反應性氣體以該真空容器內之壓力達到目標壓力之方式進行控制並導入,對設置於該陰極之鋁靶進行濺鍍,於與該鋁靶對向之矽基板上形成氧化膜;且包括如下構件:電漿產生氣體導入部,其將上述濺鍍氣體及上述反應性氣體導入至上述真空容器內;控制部,其控制藉由上述電漿產生氣體導入部導入至上述處理空間之上述反應性氣體之導入量;高頻天線,其設置於上述真空容器內且包含卷數未達一圈之導體;高頻電源,其對上述高頻天線供給高頻電力,以使得於導入有上述濺鍍氣體及上述反應性氣體之上述真空容器內產生高頻電感耦合電漿;及濺鍍用電源,其對上述鋁靶施加負電壓、包含負電壓及正電壓之直流脈衝、或交流之任一種濺鍍電壓,以使得藉由上述磁控陰極所形成之靜磁場而於導入有上述濺鍍氣體及上述反應性氣體之上述真空容器內產生磁控電漿;且上述濺鍍用電源將上述濺鍍電壓進行定電壓控制;上述控制部係以流動於上述磁控陰極之濺鍍電流值達到目標電流值之方式,控制於上述磁控電漿之產生過程中上述電漿產生氣體導入部導入至上述真空容器內之上述反應性氣體之導入量。 The ninth aspect of the sputtering apparatus is controlled in a vacuum vessel provided with a magnetron cathode for forming a static magnetic field, and the reactive gas of the sputtering gas and the oxygen gas is controlled and introduced by the pressure in the vacuum vessel to reach the target pressure. Sputtering an aluminum target disposed on the cathode to form an oxide film on the substrate opposite to the aluminum target; and comprising: a plasma generating gas introduction portion that converts the sputtering gas and the reactivity a gas is introduced into the vacuum container; a control unit controls an introduction amount of the reactive gas introduced into the processing space by the plasma generating gas introduction unit; and a high frequency antenna is provided in the vacuum container and includes a roll a conductor having a number of turns; a high frequency power supply that supplies high frequency power to the high frequency antenna to generate a high frequency inductively coupled plasma in the vacuum vessel into which the sputtering gas and the reactive gas are introduced; And a power source for sputtering, which applies a negative voltage, a DC pulse including a negative voltage and a positive voltage, or a sputtering voltage to the aluminum target, so that a static magnetic field formed by the magnetron cathode generates a magnetron plasma in the vacuum vessel into which the sputtering gas and the reactive gas are introduced; and the sputtering power source controls the sputtering voltage by a constant voltage; The system controls the reactive gas introduced into the vacuum vessel by the plasma generating gas introduction portion during the generation of the magnetron plasma by the sputtering current value flowing through the magnetron cathode reaching a target current value The amount of import.

根據本發明,第1電漿產生步驟係使用設置於導入有濺鍍氣體及氧氣之反應性氣體之真空容器內且包含卷數未達一圈之導體之高頻天線,至少於第2電漿產生步驟中於真空容器內產生高頻電感耦合電 漿。而且,第2電漿產生步驟係對靶材施加濺鍍電壓並產生磁控電漿。因此,藉由氧自由基之增加、成膜對象基板上之氧化反應之促進、以及伴隨其等而產生之經氧化之靶材表面之軟化之綜合性效果,而使成膜速度高速化。又,根據本發明,於第2電漿產生步驟中將濺鍍電壓進行定電壓控制,並且以流動於磁控陰極之濺鍍電流值達到目標電流值之方式,控制第2電漿產生步驟中反應性氣體之導入量。於將濺鍍電壓進行定電壓控制之情形,即以電壓固定模式驅動濺鍍電源之情形時,形成於基板上之氧化鋁膜之氧化度係穩定於與真空容器內之氧氣量、即反應性氣體量相應之穩定之平衡點。又,於將濺鍍電壓進行定電壓控制之情形時,鋁靶表面之氧化度越高,即真空容器內之反應性氣體量越多,則濺鍍電流值變得越大,並且成膜於基板上之氧化鋁之氧化度亦變得越高。因此,根據本發明,藉由以濺鍍電流值達到目標電流值之方式將反應性氣體導入至真空容器內,無關例如由於吸附於基板之水分等而產生之反應性氣體等干擾因素,而可使形成於基板上之氧化鋁膜之氧化度穩定。即,可使氧化度穩定地、且以較快之成膜速度成膜氧化鋁。 According to the invention, the first plasma generating step uses a high-frequency antenna provided in a vacuum vessel into which a reactive gas of a sputtering gas and oxygen gas is introduced, and includes a conductor having a number of windings less than one turn, at least the second plasma High frequency inductive coupling in a vacuum vessel during the production step Pulp. Moreover, the second plasma generating step applies a sputtering voltage to the target and generates a magnetron plasma. Therefore, the film formation speed is increased by the synergistic effect of the increase in oxygen radicals, the promotion of the oxidation reaction on the substrate to be coated, and the softening of the surface of the oxidized target caused by the formation of the substrate. Further, according to the present invention, the sputtering voltage is subjected to constant voltage control in the second plasma generating step, and the second plasma generating step is controlled in such a manner that the sputtering current value flowing through the magnetron cathode reaches the target current value. The amount of introduction of reactive gas. When the sputtering voltage is controlled by constant voltage, that is, when the sputtering power source is driven in the voltage fixed mode, the oxidation degree of the aluminum oxide film formed on the substrate is stabilized in the amount of oxygen in the vacuum container, that is, the reactivity. The corresponding balance of gas levels. Moreover, when the sputtering voltage is subjected to constant voltage control, the higher the degree of oxidation of the surface of the aluminum target, that is, the greater the amount of reactive gas in the vacuum vessel, the larger the sputtering current value becomes, and the film is formed. The degree of oxidation of the alumina on the substrate also becomes higher. Therefore, according to the present invention, the reactive gas is introduced into the vacuum vessel so that the sputtering current value reaches the target current value, irrespective of, for example, a disturbance factor such as a reactive gas generated by moisture adsorbed on the substrate. The degree of oxidation of the aluminum oxide film formed on the substrate is stabilized. That is, the alumina can be formed stably at a relatively high film formation rate.

10‧‧‧濺鍍裝置 10‧‧‧ Sputtering device

11‧‧‧腔室 11‧‧‧ chamber

12‧‧‧磁控濺鍍用磁鐵 12‧‧‧ Magnets for magnetron sputtering

14‧‧‧底板(陰極) 14‧‧‧Bottom plate (cathode)

15‧‧‧基板平台 15‧‧‧Substrate platform

17‧‧‧窗部 17‧‧‧ Window Department

18‧‧‧靶材.天線配置部 18‧‧‧ Targets. Antenna configuration department

19‧‧‧電漿產生氣體導入部 19‧‧‧ Plasma generation gas introduction

20‧‧‧氣體導入口 20‧‧‧ gas inlet

24‧‧‧靶材保持部 24‧‧‧ Target Holding Department

51‧‧‧曲線 51‧‧‧ Curve

52‧‧‧曲線 52‧‧‧ Curve

53‧‧‧曲線 53‧‧‧ Curve

54‧‧‧曲線 54‧‧‧ Curve

55‧‧‧曲線 55‧‧‧ Curve

60‧‧‧靶材(鋁靶) 60‧‧‧ Target (aluminum target)

74‧‧‧基板 74‧‧‧Substrate

80‧‧‧高頻天線 80‧‧‧High frequency antenna

90‧‧‧電漿產生部 90‧‧‧The Plasma Generation Department

111‧‧‧分光器 111‧‧‧ Spectroscope

112‧‧‧探針 112‧‧‧Probe

113‧‧‧處理室 113‧‧‧Processing room

151‧‧‧冷媒 151‧‧‧Refrigerant

161‧‧‧高頻電源 161‧‧‧High frequency power supply

162‧‧‧濺鍍用電源 162‧‧‧Power supply for sputtering

163‧‧‧匹配電路 163‧‧‧Matching circuit

164‧‧‧電流計 164‧‧‧ galvanometer

181‧‧‧靶材配置塊 181‧‧‧target configuration block

182‧‧‧天線固定塊 182‧‧‧Antenna fixed block

189‧‧‧陽極 189‧‧‧Anode

191‧‧‧反應性氣體供給部 191‧‧‧Reactive Gas Supply Department

192‧‧‧流量控制器 192‧‧‧Flow Controller

200‧‧‧控制部 200‧‧‧Control Department

351‧‧‧閘極 351‧‧‧ gate

411‧‧‧保護管 411‧‧‧Protection tube

601‧‧‧虛線框 601‧‧‧dotted box

602‧‧‧虛線框 602‧‧‧dotted box

603‧‧‧虛線框 603‧‧‧dotted box

G1‧‧‧曲線 G1‧‧‧ curve

G2‧‧‧曲線 G2‧‧‧ curve

G3‧‧‧曲線 G3‧‧‧ Curve

Ia‧‧‧目標電流值 Ia‧‧‧target current value

L1‧‧‧虛線 L1‧‧‧ dotted line

L2‧‧‧虛線 L2‧‧‧ dotted line

L3‧‧‧虛線 L3‧‧‧ dotted line

L4‧‧‧虛線 L4‧‧‧ dotted line

L11‧‧‧曲線 L11‧‧‧ curve

S1‧‧‧點 S1‧‧ points

S2‧‧‧點 S2‧‧ points

S3‧‧‧點 S3‧‧ points

S110‧‧‧步驟 S110‧‧‧Steps

S120‧‧‧步驟 S120‧‧‧ steps

S130‧‧‧步驟 S130‧‧‧Steps

S140‧‧‧步驟 S140‧‧‧Steps

S150‧‧‧步驟 S150‧‧ steps

S160‧‧‧步驟 S160‧‧‧ steps

S170‧‧‧步驟 S170‧‧‧Steps

S180‧‧‧步驟 S180‧‧‧Steps

S190‧‧‧步驟 S190‧‧ steps

S200‧‧‧步驟 S200‧‧‧ steps

S210‧‧‧步驟 S210‧‧‧Steps

S220‧‧‧步驟 S220‧‧‧Steps

T21‧‧‧時間 T21‧‧‧ time

t0‧‧‧時間 Time t0‧‧‧

t1‧‧‧時間 Time t1‧‧‧

t2‧‧‧時間 Time t2‧‧‧

t3‧‧‧時間 Time t3‧‧‧

t4‧‧‧時間 Time t4‧‧‧

t5‧‧‧時間 Time t5‧‧‧

t6‧‧‧時間 Time t6‧‧‧

t7‧‧‧時間 Time t7‧‧‧

t8‧‧‧時間 Time t8‧‧‧

t9‧‧‧時間 Time t9‧‧‧

X‧‧‧軸 X‧‧‧ axis

Y‧‧‧軸 Y‧‧‧ axis

Z‧‧‧軸 Z‧‧‧ axis

圖1係例示實現實施形態之氧化鋁之成膜方法之濺鍍裝置之主要部分之概略構成的圖。 Fig. 1 is a view showing a schematic configuration of a main part of a sputtering apparatus for realizing a film forming method of alumina according to an embodiment.

圖2係表示高頻天線之例之側視圖。 Fig. 2 is a side view showing an example of a high frequency antenna.

圖3係用以說明利用實施形態之氧化鋁之成膜方法之成膜之過程的模式圖。 Fig. 3 is a schematic view for explaining a process of film formation by the film forming method of alumina of the embodiment.

圖4係模式性地表示實施形態之氧化鋁之成膜方法之效果的圖。 Fig. 4 is a view schematically showing the effect of the film forming method of alumina in the embodiment.

圖5係實驗實施形態之氧化鋁之成膜方法時之時間圖之一例。 Fig. 5 is a view showing an example of a time chart in the film formation method of alumina in the experimental embodiment.

圖6係例示實施形態之氧化鋁之成膜方法之順序之流程圖。 Fig. 6 is a flow chart showing the procedure of the film forming method of alumina in the embodiment.

圖7係例示實施形態之氧化鋁之成膜方法之順序之流程圖。 Fig. 7 is a flow chart showing the procedure of the film forming method of alumina in the embodiment.

圖8係模式性地表示濺鍍電流值與反應性氣體之電漿發光強度之關係的圖。 Fig. 8 is a view schematically showing the relationship between the sputtering current value and the plasma luminous intensity of the reactive gas.

圖9係模式性地表示使用濺鍍電流值之變化之預測的反應性氣體之導入量之控制例的圖。 Fig. 9 is a view schematically showing an example of control of the amount of introduction of the reactive gas using the predicted change in the sputtering current value.

以下,基於圖式,說明本發明之一實施形態。於圖式中係對具有相同之構成及功能之部分標附相同符號,且於下述說明中省略重複說明。又,各圖式係模式性地予以表示,例如各圖式中表示物之尺寸及位置關係等未必被準確地圖示。又,於一部分圖式中,為說明方向而標附有XYZ正交座標軸。該座標軸中Z軸之方向表示鉛垂線之方向,XY平面為水平面。 Hereinafter, an embodiment of the present invention will be described based on the drawings. In the drawings, the same reference numerals are given to the parts having the same configurations and functions, and the repeated description is omitted in the following description. Further, each drawing is schematically shown, and for example, the size and positional relationship of the objects in the respective drawings are not necessarily accurately shown. Further, in a part of the drawings, an XYZ orthogonal coordinate axis is attached to explain the direction. The direction of the Z axis in the coordinate axis indicates the direction of the vertical line, and the XY plane is the horizontal plane.

<關於實施形態:> <About the implementation form:> <1.濺鍍裝置之構成> <1. Composition of sputtering device>

圖1係例示實現實施形態之氧化鋁之成膜方法之濺鍍裝置10之主要部分之概略構成的圖。圖2係表示高頻天線80之例之側視圖。以下,參照圖1、圖2,對濺鍍裝置10之構成進行說明。 Fig. 1 is a view showing a schematic configuration of a main part of a sputtering apparatus 10 for realizing a film forming method of alumina according to an embodiment. FIG. 2 is a side view showing an example of the high frequency antenna 80. Hereinafter, the configuration of the sputtering apparatus 10 will be described with reference to Figs. 1 and 2 .

濺鍍裝置10係用以藉由離子而對板狀之單金屬之鋁靶(亦簡稱為「靶材」)60進行濺鍍而於基板74之表面形成特定之薄膜之裝置。鋁為導電性。 The sputtering apparatus 10 is a device for sputtering a plate-shaped single metal aluminum target (also simply referred to as "target") 60 by ions to form a specific thin film on the surface of the substrate 74. Aluminum is electrically conductive.

濺鍍裝置10包括如下構件:腔室(「真空容器」)11,其可藉由真空泵(未圖示)使內部成為真空;電漿產生氣體導入部19,其將電漿產生氣體導入至經真空排氣之腔室11內;靶材保持部24,其設置於腔室11內且保持靶材60;基板平台15,其保持成膜對象之基板74;及濺鍍用電源162。又,濺鍍裝置10進而包括如下構件:控制部200,其具備電腦等且總括控制濺鍍裝置10之各部之動作;反應性氣體供給部191,其將氧氣之反應性氣體供給至腔室11內;流量控制器192,其設 置於反應性氣體供給部191之配管路徑中;分光器111,其可測定入射至光纖探針之光之分光強度。控制部200與濺鍍裝置10之各部電性連接,且下述目標電流值等控制濺鍍裝置10所必需之各種資訊預先記憶於控制部200內之記憶部中。 The sputtering apparatus 10 includes a member ("vacuum container") 11 which can be vacuumed by a vacuum pump (not shown); the plasma generates a gas introduction portion 19 which introduces a plasma generating gas into the The inside of the chamber 11 for vacuum evacuation; the target holding portion 24, which is disposed in the chamber 11 and holds the target 60; the substrate stage 15, which holds the substrate 74 of the film formation target; and a power source 162 for sputtering. Further, the sputtering apparatus 10 further includes a control unit 200 including a computer or the like and collectively controlling the operation of each unit of the sputtering apparatus 10, and a reactive gas supply unit 191 for supplying a reactive gas of oxygen to the chamber 11. Internal; flow controller 192, which is designed The light is placed in the piping path of the reactive gas supply unit 191, and the beam splitter 111 measures the intensity of the light incident on the fiber probe. The control unit 200 is electrically connected to each of the sputtering apparatus 10, and various information necessary for controlling the sputtering apparatus 10 such as a target current value is stored in advance in the memory unit in the control unit 200.

基板平台15係以保持於靶材保持部24之靶材60之表面(+Z側之面)與基板74之表面(-Z側之面)隔開特定之距離而對向之方式保持基板74。於基板74之正下方(緊靠基板74之-Z側之附近),可開閉之省略圖示之成膜擋板至少遍及基板74之全域而設置。又,濺鍍用電源162藉由對底板(「陰極」)14施加負電壓之直流之濺鍍電壓(「陰極外加電壓」、「偏壓電壓」)、或包含負電壓及正電壓之脈衝狀之濺鍍電壓(「脈衝直流電壓」)、或者交流之濺鍍電壓,而於靶材60及保持於基板平台15之基板74之間產生磁控電漿用之電場。濺鍍用電源162係以電壓固定模式被驅動,自濺鍍用電源162之電壓輸出係以成為定電壓之方式被控制。即,濺鍍用電源162將濺鍍電壓進行定電壓控制。流動於下述磁控陰極之濺鍍電流值(「偏壓電流值」)由設置於濺鍍用電源162之電流計164檢測,並供給至控制部200。藉由使氧化鋁之成膜過程中鋁靶60之表面之氧化度(「氧化率」、「氧化狀態」)穩定,而可形成高品質之鈍化膜。若進行定電壓控制,則與進行定電力控制之情形相比,可容易使所要成膜之氧化鋁之氧化度穩定。又,基板平台15具備省略圖示之加熱器或冷卻機構,控制基板74之溫度。 The substrate stage 15 holds the substrate 74 in a manner opposed to the surface (the surface on the +Z side) of the target 60 held by the target holding portion 24 and the surface (the surface on the -Z side) of the substrate 74 by a specific distance. . Immediately below the substrate 74 (near the -Z side of the substrate 74), a film-forming baffle (not shown) that can be opened and closed is provided over at least the entire area of the substrate 74. Further, the sputtering power supply 162 is provided with a DC sputtering voltage ("cathode applied voltage", "bias voltage") for applying a negative voltage to the bottom plate ("cathode") 14, or a pulse containing a negative voltage and a positive voltage. The sputtering voltage ("pulse DC voltage") or the AC sputtering voltage generates an electric field for the magnetron plasma between the target 60 and the substrate 74 held on the substrate stage 15. The sputtering power source 162 is driven in a voltage-fixed mode, and the voltage output from the sputtering power source 162 is controlled so as to be a constant voltage. That is, the sputtering power source 162 performs constant voltage control of the sputtering voltage. The sputtering current value ("bias current value") flowing through the magnetron cathode described below is detected by the ammeter 164 provided in the sputtering power source 162, and supplied to the control unit 200. A high-quality passivation film can be formed by stabilizing the oxidation degree ("oxidation rate" and "oxidation state") of the surface of the aluminum target 60 during the film formation of alumina. When the constant voltage control is performed, the degree of oxidation of the alumina to be film-formed can be easily stabilized as compared with the case where constant power control is performed. Further, the substrate stage 15 is provided with a heater or a cooling mechanism (not shown) to control the temperature of the substrate 74.

又,濺鍍裝置10進而具備電漿產生部90,該電漿產生部90產生導入至腔室11內之電漿產生氣體之高頻電感耦合電漿。基板平台15經由安裝構件而設置於腔室11之上部之內壁。 Further, the sputtering apparatus 10 further includes a plasma generating unit 90 that generates a high-frequency inductive coupling plasma of the plasma generating gas introduced into the chamber 11. The substrate stage 15 is provided on the inner wall of the upper portion of the chamber 11 via a mounting member.

又,電漿產生部90具備不接觸靶材60之側面而沿該側面所配置之線狀高頻天線(「電漿源」)80。高頻天線80係由金屬製管狀導體所構成。而且,電漿產生部90藉由高頻天線80而產生濺鍍氣體與反應性 氣體各自之高頻電感耦合電漿。 Further, the plasma generating unit 90 includes a linear high-frequency antenna ("plasma source") 80 disposed along the side surface without contacting the side surface of the target 60. The high frequency antenna 80 is composed of a metal tubular conductor. Moreover, the plasma generating portion 90 generates sputtering gas and reactivity by the high frequency antenna 80. The respective high frequency inductive coupling of the gas.

而且,濺鍍裝置10藉由利用磁控電漿與高頻電感耦合電漿之混合電漿的靶材60之濺鍍而於基板74上之二維區域進行成膜,該磁控電漿係藉由下述磁控濺鍍用磁鐵12所形成之靜磁場於靶材60之表面部分產生之電漿產生氣體之磁控電漿,該高頻電感耦合電漿係電漿產生部90所產生之電漿產生氣體之高頻電感耦合電漿。 Moreover, the sputtering apparatus 10 forms a film on a two-dimensional region on the substrate 74 by sputtering using a target 60 of a mixed plasma of a magnetron plasma and a high frequency inductively coupled plasma. The magnetron generated by the static magnetic field formed by the magnetron sputtering magnet 12 is generated on the surface portion of the target 60 to generate a magnetically controlled plasma, which is generated by the high frequency inductively coupled plasma plasma generating portion 90. The plasma produces a high frequency inductively coupled plasma of the gas.

於腔室11之側面設置有可開閉之閘極351。成膜對象之基板74係自閘極351搬入至腔室11內,藉由未圖示之固定構件安裝於基板平台15之後,實施利用濺鍍之成膜,自閘極351搬出至腔室11之外部。於對基板74進行成膜時,在成膜之前,將基板74搬入至腔室11內,於閘極351被封閉之狀態下,藉由未圖示之真空泵,將作為腔室11之內部空間之處理室113真空排氣。 An openable and closable gate 351 is disposed on a side surface of the chamber 11. The substrate 74 to be film-formed is carried into the chamber 11 from the gate 351, and is attached to the substrate stage 15 by a fixing member (not shown), and then formed into a film by sputtering, and is carried out from the gate 351 to the chamber 11 External. When the substrate 74 is formed, the substrate 74 is carried into the chamber 11 before the film formation, and the internal space of the chamber 11 is opened by a vacuum pump (not shown) in a state where the gate 351 is closed. The processing chamber 113 is evacuated.

繼而,於閘極351被關閉之狀態下,電漿產生氣體自電漿產生氣體導入部19之氣體導入口20導入至腔室11內,藉此,處理室113維持於固定壓力下、固定氣體分壓下。氣體導入口20形成於例如高頻天線80與靶材60之間之部分等。於電漿產生部90具備複數個高頻天線80之情形時,氣體導入口20分別設置於例如與各高頻天線80相對應之位置。 Then, in a state where the gate 351 is closed, the plasma generating gas is introduced into the chamber 11 from the gas introduction port 20 of the plasma generating gas introduction portion 19, whereby the processing chamber 113 is maintained at a fixed pressure and fixed gas. Under partial pressure. The gas introduction port 20 is formed, for example, at a portion between the high frequency antenna 80 and the target 60. When the plasma generating unit 90 includes a plurality of high frequency antennas 80, the gas inlet ports 20 are provided at positions corresponding to the respective high frequency antennas 80, for example.

為了藉由反應性濺鍍而成膜作為鋁之氧化物之氧化鋁,濺鍍裝置10可使用為惰性氣體之Ar氣體或Kr氣體等濺鍍氣體及氧氣(O2)之反應性氣體作為電漿產生氣體。濺鍍氣體係自省略圖示之濺鍍氣體供給部經由電漿產生氣體導入部19而供給。又,電漿產生氣體導入部19係經由配管與流量控制器192連接,流量控制器192係經由配管與供給所貯存之反應性氣體之反應性氣體供給部191連接。而且,控制部200監測自濺鍍用電源162供給之濺鍍電流值,控制部200藉由控制流量控制器192,而控制自反應性氣體供給部191供給至腔室11內之反應性氣體 之導入量。又,於腔室11之側壁,設置有將腔室11內密閉並且可使腔室11內之電漿發光透過之窗部17,於窗部之附近,以電漿發光可入射之方式設置有分光器111之探針112。分光器111係構成為,至少將作為氧氣之反應性氣體之電漿發光之明線之波長的波長777nm之光進行分光,而可檢測其強度。分光器111經由窗部17而檢測之經分光之電漿之發光強度被供給至控制部200。控制部200可根據所供給之發光強度中之氧氣之反應性氣體之電漿發光之強度,而如下所述般控制反應性氣體之導入量。 In order to form a film of aluminum oxide by reactive sputtering, the sputtering apparatus 10 can use a sputtering gas such as an inert gas of Ar gas or Kr gas or a reactive gas of oxygen (O 2 ) as electricity. The slurry produces a gas. The sputtering gas system is supplied from the sputtering gas supply unit (not shown) via the plasma generation gas introduction unit 19. Further, the plasma generated gas introduction unit 19 is connected to the flow rate controller 192 via a pipe, and the flow rate controller 192 is connected to the reactive gas supply unit 191 that supplies the stored reactive gas via a pipe. Further, the control unit 200 monitors the value of the sputtering current supplied from the sputtering power source 162, and the control unit 200 controls the flow rate of the reactive gas supplied from the reactive gas supply unit 191 to the chamber 11 by controlling the flow rate controller 192. The amount of import. Further, on the side wall of the chamber 11, a window portion 17 for sealing the inside of the chamber 11 and allowing the plasma in the chamber 11 to emit light is provided, and in the vicinity of the window portion, the plasma light is incident on the surface. The probe 112 of the beam splitter 111. The spectroscope 111 is configured to split the light having a wavelength of 777 nm which is a wavelength of the bright line of the plasma which is a reactive gas of oxygen, and to detect the intensity. The luminous intensity of the spectroscopic plasma detected by the spectroscope 111 via the window portion 17 is supplied to the control unit 200. The control unit 200 can control the introduction amount of the reactive gas as follows, based on the intensity of the plasma luminescence of the reactive gas of oxygen in the supplied luminescence intensity.

於腔室11之底部設置有開口,並且以自下側堵住該開口之方式安裝有用以收容下述底板14及磁控濺鍍用磁鐵(永久磁鐵)12(統稱為磁控陰極)、以及高頻天線80之靶材.天線配置部18。靶材.天線配置部18與腔室11之底部之連接部藉由密封材料得以確保氣密性。因此,靶材.天線配置部18之壁具有作為腔室11之壁之一部分之作用。於靶材.天線配置部18,於基板平台15之正下方之位置,設置有靶材配置塊(靶材配置部)181。並且,於靶材.天線配置部18之壁內(即腔室11之壁內)且靶材配置塊181之側方,以夾著靶材配置塊181之方式設置有1對天線固定塊182。磁控陰極於靶材60之表面附近形成靜磁場。 An opening is provided at the bottom of the chamber 11, and the opening is blocked from the lower side to accommodate the bottom plate 14 and the magnetron sputtering magnet (permanent magnet) 12 (collectively referred to as a magnetron cathode), and The target of the high frequency antenna 80. Antenna arrangement unit 18. Target. The connection portion between the antenna arrangement portion 18 and the bottom portion of the chamber 11 is ensured to be airtight by the sealing material. Therefore, the target. The wall of the antenna arrangement portion 18 functions as a part of the wall of the chamber 11. For the target. The antenna arrangement portion 18 is provided with a target arrangement block (target arrangement portion) 181 at a position directly below the substrate stage 15. And, in the target. A pair of antenna fixing blocks 182 are provided in the wall of the antenna arrangement portion 18 (that is, in the wall of the chamber 11) and on the side of the target arrangement block 181 so as to sandwich the target arrangement block 181. The magnetron cathode forms a static magnetic field near the surface of the target 60.

於靶材配置塊181之上部有腔室11之處理室113。於靶材配置塊181內載置有磁控濺鍍用磁鐵12。於磁控濺鍍用磁鐵12之上表面設置有底板14,並且與底板14對向之基板平台15設置於腔室11之上側內壁。基板平台15接地。再者,基板平台15亦可為未接地之浮動狀態。磁控濺鍍用磁鐵12之上下方向之位置被調整為,設置於其上表面之底板14上所載置之靶材60之上表面配置於靶材.天線配置部18之上端附近(無需為與上端相同之位置)。又,靶材60係藉由底板14及靶材保持部24而保持於底板14之上表面(+Z側之面)。藉由如此般設置磁控濺鍍用磁鐵12及底板14(統稱為磁控陰極),而將靶材60配置於腔室11之面 向處理室113之空間內。 A processing chamber 113 of the chamber 11 is provided above the target arranging block 181. The magnetron sputtering magnet 12 is placed in the target arrangement block 181. A bottom plate 14 is disposed on the upper surface of the magnet 12 for magnetron sputtering, and a substrate platform 15 opposed to the bottom plate 14 is disposed on the upper inner wall of the chamber 11. The substrate platform 15 is grounded. Furthermore, the substrate platform 15 can also be in an ungrounded floating state. The position of the magnetron sputtering magnet 12 in the upper and lower directions is adjusted so that the upper surface of the target 60 placed on the bottom plate 14 provided on the upper surface thereof is disposed on the target. The vicinity of the upper end of the antenna arrangement portion 18 (the same position as the upper end is not required). Further, the target 60 is held by the bottom plate 14 and the target holding portion 24 on the upper surface (surface on the +Z side) of the bottom plate 14. By providing the magnetron sputtering magnet 12 and the bottom plate 14 (collectively referred to as magnetron cathodes) in this manner, the target 60 is disposed on the surface of the chamber 11. Into the space of the processing chamber 113.

磁控濺鍍用磁鐵12係於包含保持於靶材保持部24之靶材60之表面之區域形成靜磁場(磁控磁場),從而可於靶材60之表面部分形成電漿。靶材60之表面部分之電漿之擴散方式係根據導入至腔室11之電漿產生氣體之分壓、或磁控濺鍍用磁鐵12所產生之磁控磁場或對靶材賦予之電壓之強度等而變動。 The magnetron sputtering magnet 12 forms a static magnetic field (magnetostatic magnetic field) in a region including the surface of the target 60 held by the target holding portion 24, so that plasma can be formed on the surface portion of the target 60. The plasma of the surface portion of the target 60 is diffused according to the partial pressure of the plasma generated by the plasma introduced into the chamber 11, or the magnetron magnetic field generated by the magnet 12 for magnetron sputtering or the voltage applied to the target. The intensity changes and so on.

又,於靶材配置塊181上端與腔室11之處理室113之邊界,以自靶材配置塊181之側壁朝向內側延伸且對靶材60之邊緣附近(包含邊緣之部分)保持一定之距離之方式,設置有陽極189。 Further, a boundary between the upper end of the target arranging block 181 and the processing chamber 113 of the chamber 11 extends inward from the side wall of the target arranging block 181 and maintains a certain distance from the vicinity of the edge of the target 60 (including the portion of the edge). In this manner, an anode 189 is provided.

於天線固定塊182內插入有高頻天線80。又,濺鍍裝置10具備將高頻電力供給至高頻天線80之高頻電源161。高頻電源161經由匹配電路163連接於高頻天線80。 A high frequency antenna 80 is inserted into the antenna fixing block 182. Further, the sputtering apparatus 10 includes a high-frequency power source 161 that supplies high-frequency power to the high-frequency antenna 80. The high frequency power source 161 is connected to the high frequency antenna 80 via the matching circuit 163.

高頻天線80係用以支援利用磁控陰極濺鍍之電漿產生,例如,如圖2所示,將金屬製之管狀導體彎曲成U字形,於兩個天線固定塊182內,以「U」字上下逆向之狀態各立設有1個。再者,高頻天線80之配置態樣可進行多種變更。作為高頻天線80之形狀,例如亦可採用圓弧狀之形狀。又,高頻天線80之卷數未達一圈。為防止駐波之產生,高頻天線80之長度較佳為設定為高頻電源161所供給之電力之波長之1/4以下之長度。自高頻天線之一端供給高頻電力,另一端接地。藉此而產生電感耦合電漿。若採用此種高頻天線80,則與使用線圈狀(螺旋狀)之天線產生電感耦合電漿之方法相比,天線之電感較低,故而可降低天線之電壓,因此可抑制電漿損傷。又,由於將天線長度縮短至高頻之波長之1/4以下,故而可抑制起因於由駐波之影響所致之電漿不均的濺鍍不均(不均一性)。又,由於可將天線收容於腔室內,故而可提高濺鍍效率。進而,根據成膜對象之基板尺寸,增加高頻天線80之個數,並且增大靶材之尺寸,藉此,即便於基板尺寸較 大之情形時,亦可謀求濺鍍速度之提昇。 The high frequency antenna 80 is used to support the generation of plasma by magnetron sputtering. For example, as shown in FIG. 2, the tubular conductor made of metal is bent into a U shape, and the two antenna fixing blocks 182 are "U. There is one state in the state of the word upside down. Furthermore, the configuration of the high frequency antenna 80 can be variously changed. As the shape of the high-frequency antenna 80, for example, an arc shape can also be adopted. Also, the number of coils of the high frequency antenna 80 is less than one turn. In order to prevent the occurrence of the standing wave, the length of the radio-frequency antenna 80 is preferably set to be a length equal to or less than 1/4 of the wavelength of the power supplied from the high-frequency power source 161. The high frequency power is supplied from one end of the high frequency antenna and the other end is grounded. Thereby an inductively coupled plasma is produced. When such a high-frequency antenna 80 is used, the inductance of the antenna is lower than that of the method of generating an inductively coupled plasma using a coil-like (spiral) antenna, so that the voltage of the antenna can be reduced, so that plasma damage can be suppressed. Further, since the length of the antenna is shortened to 1/4 or less of the wavelength of the high frequency, it is possible to suppress sputtering unevenness (non-uniformity) due to plasma unevenness due to the influence of the standing wave. Moreover, since the antenna can be housed in the chamber, the sputtering efficiency can be improved. Further, according to the substrate size of the film formation object, the number of the high frequency antennas 80 is increased, and the size of the target material is increased, whereby even the substrate size is increased. In the case of a big situation, it is also possible to increase the sputtering speed.

U字形之高頻天線相當於卷數未達1圈之電感耦合天線,由於電感較卷數為1圈以上之電感耦合天線更低,故而降低了產生於高頻天線之兩端之高頻電壓,抑制了伴隨對於產生之電漿之電容耦合而產生之電漿電位之高頻振盪。因此,降低了伴隨向對地電位之電漿電位振盪而產生之過剩之電子損耗,降低了電漿電位。藉此,可實現基板上之低離子損傷之薄膜形成製程。構成高頻天線80之金屬製管狀導體具有於使用濺鍍裝置10時藉由將水等冷媒151通過其內部而冷卻高頻天線80之功能。高頻天線80之高度方向之位置係被調整為,「U」字之底部較與靶材60之上表面同等程度之高度高出數厘米左右,以使得靶材60之表面附近之電漿密度變得更高。再者,由於靶材60及底板14等亦會變得異常高溫,故而較佳為與高頻天線80同樣地藉由冷媒151進行冷卻。 The U-shaped high-frequency antenna is equivalent to an inductively coupled antenna with less than one turn of the coil. Since the inductance is lower than the inductive coupling antenna with more than one turn, the high-frequency voltage generated at both ends of the high-frequency antenna is reduced. The high frequency oscillation accompanying the plasma potential generated for the capacitive coupling of the generated plasma is suppressed. Therefore, the excess electron loss accompanying the oscillation of the plasma potential to the ground potential is reduced, and the plasma potential is lowered. Thereby, a film formation process with low ion damage on the substrate can be realized. The metal tubular conductor constituting the high-frequency antenna 80 has a function of cooling the high-frequency antenna 80 by passing the refrigerant 151 such as water through the inside of the sputtering apparatus 10. The position of the high-frequency antenna 80 in the height direction is adjusted such that the bottom of the "U" is about several centimeters higher than the height of the upper surface of the target 60 so that the plasma density near the surface of the target 60 is Become higher. Further, since the target 60 and the bottom plate 14 and the like are also abnormally high in temperature, it is preferable to cool the refrigerant 151 in the same manner as the high-frequency antenna 80.

高頻天線80之上端側之一部分貫通天線固定塊182,向腔室11之內部側突設。高頻天線80之該突設部分由包含石英等之介電體之保護管411覆蓋。 One of the upper end sides of the high-frequency antenna 80 penetrates the antenna fixing block 182 and protrudes toward the inner side of the chamber 11. The protruding portion of the high frequency antenna 80 is covered by a protective tube 411 containing a dielectric such as quartz.

再者,磁控濺鍍用磁鐵12於靶材60表面之水平磁通密度之最大值為20至50mT(毫特斯拉(millitesla)),即便為較無高頻電感耦合天線之支援之情形時之磁通密度(60至100mT)更低之磁通密度,亦可產生充分之電漿。 Furthermore, the maximum value of the horizontal magnetic flux density of the magnetron sputtering magnet 12 on the surface of the target 60 is 20 to 50 mT (millitesla), even in the case of support without a high frequency inductive coupling antenna. A lower magnetic flux density (60 to 100 mT) can also produce sufficient plasma.

基板平台15可藉由設置於基板平台15之下表面之省略圖示之爪狀構件等而保持基板74。基板74例如包含矽晶圓等。 The substrate stage 15 can hold the substrate 74 by a claw-shaped member or the like (not shown) provided on the lower surface of the substrate stage 15. The substrate 74 includes, for example, a germanium wafer or the like.

如上所述般構成之濺鍍裝置10係將濺鍍氣體及氧氣之反應性氣體導入至設置有底板14之腔室11,並對設置於該陰極之鋁靶60進行濺鍍,於與該靶材60對向之基板74上成膜氧化鋁。 The sputtering apparatus 10 configured as described above introduces a sputtering gas and a reactive gas of oxygen into the chamber 11 provided with the bottom plate 14, and sputters the aluminum target 60 provided on the cathode to be used with the target. Aluminium 60 is formed on the substrate 74 opposite to the substrate 74.

<2.關於氧化鋁之成膜過程> <2. About the film formation process of alumina>

圖3係用以說明可預測到於利用實施形態之氧化鋁之成膜方法之成膜過程中更多地產生之現象的模式圖。圖4係模式性地表示實施形態之氧化鋁之成膜方法之效果之圖。圖4之曲線G1表示通常(未進行基於高頻電感耦合電漿之電漿產生之支援之情形時)之基於反應性磁控濺鍍之氧化鋁(Al2O3)之成膜速度與氧氣量之關係。曲線G2、G3表示進行基於高頻電感耦合電漿之電漿產生之支援之本實施形態之氧化鋁之成膜方法的成膜速度與氧氣量之關係。曲線G2與施加負電壓之直流電壓作為濺鍍電壓之情形相對應,曲線G3與施加脈衝直流電壓或交流電壓作為濺鍍電壓之情形相對應。 Fig. 3 is a schematic view for explaining a phenomenon which is more likely to occur in the film formation process by the film formation method of alumina using the embodiment. Fig. 4 is a view schematically showing the effect of the film forming method of alumina in the embodiment. The curve G1 of Fig. 4 shows the film formation speed and oxygen of the reactive magnetron sputtering-based alumina (Al 2 O 3 ) in the usual case (when the support of the plasma generation by the high-frequency inductively coupled plasma is not performed). The relationship between quantity. Curves G2 and G3 indicate the relationship between the film formation speed and the amount of oxygen in the film formation method of alumina according to the present embodiment, which is supported by plasma generation of high-frequency inductively coupled plasma. The curve G2 corresponds to a case where a DC voltage to which a negative voltage is applied is used as a sputtering voltage, and a curve G3 corresponds to a case where a pulsed DC voltage or an AC voltage is applied as a sputtering voltage.

<2-1.關於成膜速度之高速化> <2-1. About the speed of film formation speed>

於通常(未進行基於高頻電感耦合電漿之電漿產生之支援之情形時)之利用反應性磁控濺鍍之氧化鋁(Al2O3)之成膜過程中,若腔室11內之氧分壓增加,則促進靶材60之表面上之氧化反應。若進而增加氧分壓,則其表面大致由化學計量之氧化鋁(Al2O3)覆蓋。由於化學計量之氧化鋁硬度較高,故而濺鍍產率降低,結果,成膜速度降低(包含較圖4之曲線G1之虛線L1更靠紙面右側之點S1之區域)。 In the film formation process of the reactive magnetron sputtering alumina (Al 2 O 3 ) in the usual (when the support of the plasma generation based on the high-frequency inductively coupled plasma is not performed), if the chamber 11 is inside The increase in oxygen partial pressure promotes the oxidation reaction on the surface of the target 60. If the partial pressure of oxygen is further increased, the surface is substantially covered by stoichiometric alumina (Al 2 O 3 ). Since the stoichiometric alumina hardness is high, the sputtering yield is lowered, and as a result, the film formation speed is lowered (including the region of the point S1 on the right side of the paper surface from the broken line L1 of the curve G1 of Fig. 4).

由虛線框601~603(圖3)包圍之模式圖分別表示氧化鋁(Al2O3)之成膜過程之一部分,該氧化鋁(Al2O3)之成膜過程之一部分係可預測到產生於實施形態之氧化鋁之成膜方法、即進行基於藉由高頻天線80產生之高頻電感耦合電漿的電漿產生之支援的反應性磁控濺鍍時。再者,亦可預測到於該情形時,亦產生了通常之反應性磁控濺鍍之上述產生過程。 By dashed boxes 601 through 603 (FIG. 3) surrounds a portion of the schematic diagram, respectively forming aluminum oxide (Al 2 O 3) of the process, a portion of the alumina-based (Al 2 O 3) of the deposition process can be predicted The method of forming a film of alumina according to the embodiment, that is, performing reactive magnetron sputtering supported by plasma generation by high-frequency inductively coupled plasma generated by the high-frequency antenna 80. Furthermore, it is also predicted that in this case, the above-described generation process of the usual reactive magnetron sputtering is also produced.

根據進行基於高頻電感耦合電漿之電漿產生之支援的本實施形態之氧化鋁之成膜方法,即便施加負電壓之直流電壓、包含負電壓及正電壓之脈衝直流電壓、或者交流電壓之任一者作為濺鍍電壓,亦可充分地提高高頻電感耦合電漿之密度。而且,於處理室113內,與離 子相比,自由基變得異常多。而且,氧自由基積極地作用於成膜對象之基板74表面,藉此而促進了基板74表面之化學計量之氧化鋁(Al2O3)之產生。如此,基於氧自由基之基板74表面之氧化得以促進之結果(虛線框602內之模式圖)為,靶材表面可選擇較低之氧氣之添加量之濺鍍條件,因而促進了氧化度低於化學計量之氧化度之氧化鋁、即非化學計量之氧化鋁(AlO)之狀態下之濺鍍,從而使靶材表面軟化(虛線框601內之模式圖)。即,靶材表面成為較低之氧化度之軟化狀態之氧化鋁,濺鍍產率提昇,另一方面,自靶材所濺鍍之AlO粒子藉由所增加之氧自由基而於成膜對象基板之表面上或基板與靶材間之真空空間變化為化學計量之氧化鋁(Al2O3),從而於基板上成膜(虛線框602內之模式圖)。因此,成膜對象之基板表面之氧化鋁之成膜速度與無基於高頻電感耦合電漿之電漿產生之支援之通常之反應性磁控濺鍍相比高速化(包含圖4之曲線G2之點S2之虛線L2與虛線L3間之區域、及包含曲線G3之點S3之虛線L3與虛線L4間之區域)。 According to the method for forming a film of alumina according to the present embodiment, which is supported by plasma generation of high-frequency inductively coupled plasma, even a DC voltage of a negative voltage, a pulsed DC voltage including a negative voltage and a positive voltage, or an AC voltage is applied. Either one of the sputtering voltages can sufficiently increase the density of the high frequency inductively coupled plasma. Further, in the processing chamber 113, radicals become abnormally larger than ions. Further, oxygen radicals actively act on the surface of the substrate 74 of the film formation object, thereby promoting the generation of the stoichiometric amount of alumina (Al 2 O 3 ) on the surface of the substrate 74. Thus, the result of the oxidation of the surface of the oxygen radical-based substrate 74 is promoted (the pattern diagram in the dashed box 602), and the surface of the target can be selected with a lower amount of oxygen added to the sputtering condition, thereby promoting a low degree of oxidation. Sputtering in the state of stoichiometric oxidation of alumina, i.e., non-stoichiometric alumina (AlO), softens the surface of the target (pattern diagram within dashed box 601). That is, the surface of the target becomes a soft state of alumina having a lower degree of oxidation, and the sputtering yield is improved. On the other hand, the AlO particles sputtered from the target are formed by the added oxygen radicals. The vacuum space on the surface of the substrate or between the substrate and the target is changed to stoichiometric alumina (Al 2 O 3 ) to form a film on the substrate (schematic diagram in the dashed box 602). Therefore, the deposition rate of the aluminum oxide on the substrate surface of the film formation object is higher than that of the conventional reactive magnetron sputtering which is not supported by the plasma generation of the high frequency inductively coupled plasma (including the curve G2 of FIG. 4). A region between the broken line L2 and the broken line L3 at the point S2, and a region between the broken line L3 and the broken line L4 including the point S3 of the curve G3.

再者,根據施加脈衝直流電壓、或者交流電壓作為濺鍍電壓之本實施形態之氧化鋁之成膜方法,將包含負電壓及正電壓之電壓施加於靶材。伴隨著施加負直流電壓之情形時之效果、以及將電子引向靶材表面之效果,藉由靶材表面之氧自由基,進一步促進利用靶材表面之化學反應之軟化(虛線框603內之模式圖),從而進一步促進自靶材表面之非化學計量之AlO之濺鍍。藉此,靶材之濺鍍產率進一步提昇,並且可抑制靶材上氧化膜之形成。因此,根據施加脈衝直流電壓、或者交流電壓作為濺鍍電壓之本實施形態之氧化鋁之成膜方法,存在基於高頻電感耦合電漿之電漿產生之支援,且相較於施加負直流電壓作為濺鍍電壓之本實施形態之氧化鋁之成膜方法,可使成膜速度進一步高速化(包含圖4之曲線G3之對應於最快之成膜速度之點S3的虛線L3與虛線L4間之區域)。 Further, a method of forming a film of alumina according to the present embodiment in which a pulsed direct current voltage or an alternating current voltage is applied as a sputtering voltage is applied to a target material with a voltage including a negative voltage and a positive voltage. With the effect of applying a negative DC voltage and the effect of directing electrons to the surface of the target, the softening of the chemical reaction using the surface of the target is further promoted by the oxygen radicals on the surface of the target (in the dashed box 603) Pattern diagram) to further promote non-stoichiometric AlO sputtering from the surface of the target. Thereby, the sputtering yield of the target is further improved, and the formation of an oxide film on the target can be suppressed. Therefore, according to the method for forming a film of alumina according to the embodiment in which a pulsed direct current voltage or an alternating current voltage is applied as a sputtering voltage, there is support for plasma generation based on high-frequency inductively coupled plasma, and compared with application of a negative direct current voltage. As a method of forming a film of alumina according to the embodiment of the sputtering voltage, the film forming speed can be further increased (including the dotted line L3 and the broken line L4 at the point S3 corresponding to the fastest film forming speed of the curve G3 of Fig. 4; Area).

<2-2.關於氧化度之穩定化> <2-2. Stabilization of oxidation degree>

於濺鍍裝置10中,在磁控電漿之產生處理中將濺鍍電壓進行定電壓控制,並且於磁控電漿之產生處理中藉由控制部200以流動於磁控陰極之濺鍍電流值達到目標電流值之方式而控制反應性氣體導入至腔室11內之導入量。具體而言,基於自檢測出之濺鍍電流值減去目標電流值所得之差值而進行如下處理:若差之符號為正,則根據差值減少反應性氣體之導入量,若差之符號為負,則根據差值增加反應性氣體之導入量。所要加減之導入量之值係例如由控制部200藉由參照預先記憶於控制部200之記憶部之運算公式、或表示對應關係之表格等而求出。 In the sputtering apparatus 10, the sputtering voltage is subjected to constant voltage control in the generation process of the magnetron plasma, and the sputtering current flowing through the magnetron cathode by the control unit 200 in the process of generating the magnetron plasma The amount of introduction of the reactive gas into the chamber 11 is controlled in such a manner that the value reaches the target current value. Specifically, based on the difference between the detected sputtering current value and the target current value, the following processing is performed: if the sign of the difference is positive, the amount of introduction of the reactive gas is reduced according to the difference, and the sign of the difference is If it is negative, the amount of introduction of the reactive gas is increased according to the difference. The value of the introduction amount to be added or subtracted is obtained, for example, by the control unit 200 by referring to an operation formula previously stored in the memory unit of the control unit 200, a table indicating the correspondence relationship, or the like.

於將濺鍍電壓進行定電壓控制之情形時,即以電壓固定模式驅動濺鍍用電源162之情形時,形成於基板74上之氧化鋁膜之氧化度穩定於與腔室11內之氧氣量、即反應性氣體量相應之穩定之平衡點。 When the sputtering voltage is subjected to constant voltage control, that is, when the sputtering power source 162 is driven in the voltage fixed mode, the oxidation degree of the aluminum oxide film formed on the substrate 74 is stabilized by the amount of oxygen in the chamber 11. That is, the equilibrium point of the corresponding amount of reactive gas.

又,靶材60之表面之氧化度越高,則靶材60於被濺鍍時會釋放出越多之二次電子。藉此,於將濺鍍電壓進行定電壓控制之情形時,靶材60表面之氧化度越高,即腔室11內之反應性氣體量越多,則濺鍍電流值變得越大,並且成膜於基板74上之氧化鋁之氧化度亦變得越高。 Moreover, the higher the degree of oxidation of the surface of the target 60, the more secondary electrons are released by the target 60 when it is sputtered. Therefore, when the sputtering voltage is subjected to constant voltage control, the higher the degree of oxidation of the surface of the target 60, that is, the larger the amount of reactive gas in the chamber 11, the larger the sputtering current value becomes, and The degree of oxidation of the alumina formed on the substrate 74 also becomes higher.

因此,藉由以濺鍍電流值達到目標電流值之方式將反應性氣體導入至腔室11內,無關例如由於吸附於基板74之水分等而產生之反應性氣體等干擾因素,而可使形成於基板74上之氧化鋁膜之氧化度穩定。即,可使氧化度穩定地、且以較快之成膜速度於基板74之表面成膜氧化鋁。 Therefore, by introducing the reactive gas into the chamber 11 so that the sputtering current value reaches the target current value, regardless of interference factors such as reactive gases generated by moisture adsorbed on the substrate 74, etc., it is possible to form. The degree of oxidation of the aluminum oxide film on the substrate 74 is stable. That is, the alumina can be formed on the surface of the substrate 74 stably and at a relatively high deposition rate.

又,於控制反應性氣體之導入量時所參照之目標電流值較佳為設定為所要成膜之氧化鋁之氧化度成為如下氧化度時之濺鍍電流值,即化學計量之氧化鋁與氧化度較化學計量之氧化鋁低之氧化鋁各自之 氧化度之邊界附近的氧化度。 Further, the target current value to be referred to when controlling the introduction amount of the reactive gas is preferably set to a sputtering current value when the degree of oxidation of the alumina to be formed becomes the following oxidation degree, that is, stoichiometric alumina and oxidation. Each of the aluminas having a lower stoichiometric amount of alumina The degree of oxidation near the boundary of the degree of oxidation.

此處,於圖4中,於較虛線L3更靠紙面右側區域之氧氣量時,於基板74表面產生化學計量之氧化鋁(Al2O3),於較虛線L3更靠紙面左側區域之氧氣量時,產生非化學計量之氧化鋁(AlO)。而且可知,當成膜於基板74之表面之氧化鋁之氧化度以例如圖4之虛線L3附近之點S2之成膜條件般成為如下氧化度,即化學計量之氧化鋁及氧化度較化學計量之氧化鋁低之氧化鋁各自之氧化度之邊界附近的氧化度時,成膜發揮較佳之鈍化效果之氧化鋁。 Here, in FIG. 4, when the amount of oxygen in the region on the right side of the paper is more than the broken line L3, a stoichiometric amount of alumina (Al 2 O 3 ) is generated on the surface of the substrate 74, and oxygen is located on the left side of the paper surface than the broken line L3. When measured, non-stoichiometric alumina (AlO) is produced. Further, it is understood that the degree of oxidation of the alumina formed on the surface of the substrate 74 is, for example, the film formation condition at a point S2 near the dotted line L3 in Fig. 4, that is, the stoichiometric amount of alumina and the degree of oxidation are more stoichiometric. When the degree of oxidation near the boundary of the oxidation degree of each of the alumina having a low alumina is formed, the film is formed into a alumina which exhibits a preferable passivation effect.

因此,與濺鍍裝置10之目標電流值相對應之氧化鋁之氧化度為氧化鋁之鈍化效果變高之氧化度,並且亦為成膜速度較快之氧化度。因此,能夠以較快之成膜速度穩定地成膜適於p型矽基板之鈍化膜且發揮較高之鈍化效果之氧化鋁。 Therefore, the degree of oxidation of the alumina corresponding to the target current value of the sputtering apparatus 10 is an oxidation degree at which the passivation effect of alumina becomes high, and is also a degree of oxidation at a faster film formation speed. Therefore, alumina which is suitable for a passivation film of a p-type germanium substrate and exhibits a high passivation effect can be stably formed at a relatively high film formation speed.

<3.濺鍍裝置之動作> <3. Action of Sputtering Device>

圖6、圖7係例示實施形態之氧化鋁之成膜方法之順序之流程圖。濺鍍裝置10係藉由磁控濺鍍用磁鐵(永久磁鐵)12於靶材60之附近形成靜磁場。又,圖5係藉由實驗而實現實施形態之氧化鋁之成膜方法時之時間圖之一例。 Fig. 6 and Fig. 7 are flowcharts showing the procedure of the film forming method of alumina in the embodiment. The sputtering apparatus 10 forms a static magnetic field in the vicinity of the target 60 by a magnet for magnetron sputtering (permanent magnet) 12. Moreover, FIG. 5 is an example of a time chart in the case of realizing the film formation method of the alumina of the embodiment by experiment.

首先,關閉省略圖示之成膜擋板之後,將靶材60與基板74自閘極351搬入至腔室11之處理室113內。繼而,將基板74、靶材60分別安裝於基板平台15、底板14,封閉閘極351(步驟S110,圖5之時間t0)。再者,於封閉閘極351後,將處理室113內之溫度調整為特定之溫度。 First, after the film formation shutter (not shown) is closed, the target 60 and the substrate 74 are carried from the gate 351 into the processing chamber 113 of the chamber 11. Then, the substrate 74 and the target 60 are attached to the substrate stage 15 and the bottom plate 14, respectively, and the gate 351 is closed (step S110, time t0 in FIG. 5). Furthermore, after the gate 351 is closed, the temperature in the processing chamber 113 is adjusted to a specific temperature.

其次,藉由真空泵使腔室11內成為真空之後,以腔室11之處理室113達到目標壓力之方式,經由電漿產生氣體導入部19,開始向腔室11內導入包含Ar等惰性氣體之濺鍍氣體(步驟S120,圖5之時間t1)。作為目標壓力,較佳為採用0.2Pa以上且7Pa以下之壓力。進而較佳為採用0.4Pa以上且2Pa以下之壓力。然而,目標壓力並不限定於該等 壓力,亦可採用範圍更廣之壓力。又,於目標壓力為3Pa以下之情形時,此後,為點燃之後之高頻電感耦合電漿,亦存在追加暫時將成膜室之壓力提高至3Pa以上之步驟之情形。其原因在於,使用該天線之高頻電感耦合電漿有於3Pa以下之壓力下難以點燃之特性。再者,一旦電漿點燃,即便其後恢復至較低之壓力(目標壓力),電漿亦可繼續產生。 Then, after the inside of the chamber 11 is evacuated by the vacuum pump, the gas is introduced into the chamber 11 via the plasma generating gas introduction portion 19 so that the processing chamber 113 of the chamber 11 reaches the target pressure, and the introduction of the inert gas such as Ar into the chamber 11 is started. The gas is sputtered (step S120, time t1 of Fig. 5). As the target pressure, it is preferred to use a pressure of 0.2 Pa or more and 7 Pa or less. Further, it is preferable to use a pressure of 0.4 Pa or more and 2 Pa or less. However, the target pressure is not limited to these Pressure can also be used with a wider range of pressures. In the case where the target pressure is 3 Pa or less, the high-frequency inductively coupled plasma after ignition may be added to the step of temporarily increasing the pressure in the film forming chamber to 3 Pa or more. The reason for this is that the high-frequency inductively coupled plasma using the antenna has a characteristic that it is difficult to ignite under a pressure of 3 Pa or less. Furthermore, once the plasma is ignited, the plasma can continue to be produced even after returning to a lower pressure (target pressure).

繼而,進行電漿產生處理(「第1電漿產生處理」)步驟,其係藉由將高頻電力自高頻電源161輸入至高頻天線80(步驟S130,圖5之時間t2),於高頻天線80之周圍形成高頻電感磁場,從而產生濺鍍氣體之高頻電感耦合電漿。於之後的處理步驟中,若將氧氣之反應性氣體供給至腔室11內,則第1電漿產生步驟亦會產生反應性氣體之高頻電感耦合電漿。高頻電力之供給持續至氧化鋁之成膜處理結束為止。 Then, a plasma generation process ("first plasma generation process") is performed by inputting high frequency power from the high frequency power source 161 to the high frequency antenna 80 (step S130, time t2 of FIG. 5). A high frequency inductive magnetic field is formed around the high frequency antenna 80 to generate a high frequency inductively coupled plasma of the sputtering gas. In the subsequent processing step, if oxygen reactive gas is supplied into the chamber 11, the first plasma generating step also generates a high frequency inductively coupled plasma of the reactive gas. The supply of the high-frequency power continues until the film formation process of the alumina is completed.

繼而,藉由利用底板14與濺鍍用電源162施加(偏壓之施加)包含負電壓之直流電壓之濺鍍電壓、包含負電壓及正電壓之脈衝狀之濺鍍電壓、或者交流之濺鍍電壓,而進行濺鍍電壓施加處理(步驟S140,圖5之時間t3)。藉此,進行磁控電漿產生處理(「第2電漿產生處理」)。再者,於採用負電壓之直流電壓作為濺鍍電壓之情形時,更加抑制界面之損傷,並且可於基板74上成膜氧化鋁。又,作為脈衝直流電壓與交流電壓之頻率,例如採用20~100KHz,亦可採用其他頻率。濺鍍電壓較佳為其負電壓之絕對值為100V以上且控制為300V以下(負電壓為-100V以下且-300V以上),進而更佳為150V以上且控制為250V以下(負電壓為-150V以下且-250V以上)。然而,濺鍍電壓之範圍並不限定於該等範圍內,亦可採用更廣範圍之電壓。於之後的處理步驟中,若將反應性氣體供給至腔室11內,則第2電漿產生步驟亦會產生反應性氣體之磁控電漿。又,濺鍍電壓之施加處理持續至氧化鋁之成膜處理結束為止。 Then, by using the substrate 14 and the sputtering power source 162 (applying a bias voltage), a sputtering voltage including a DC voltage of a negative voltage, a sputtering voltage including a negative voltage and a positive voltage, or a sputtering of an alternating current. The voltage is applied to the sputtering voltage application process (step S140, time t3 of Fig. 5). Thereby, a magnetron plasma generation process ("second plasma generation process") is performed. Further, when a DC voltage of a negative voltage is used as the sputtering voltage, damage to the interface is further suppressed, and alumina can be formed on the substrate 74. Further, as the frequency of the pulsed direct current voltage and the alternating current voltage, for example, 20 to 100 kHz is used, and other frequencies may be used. The sputtering voltage is preferably such that the absolute value of the negative voltage is 100 V or more and the control is 300 V or less (negative voltage is -100 V or less and -300 V or more), and more preferably 150 V or more and controlled to 250 V or less (negative voltage is -150 V) The following is -250V or more). However, the range of the sputtering voltage is not limited to these ranges, and a wider range of voltages can be used. In the subsequent processing step, when the reactive gas is supplied into the chamber 11, the second plasma generating step also generates a magnetron plasma of the reactive gas. Further, the application process of the sputtering voltage is continued until the film formation process of the aluminum oxide is completed.

其次,於控制部200所監測之濺鍍電流值成為低於特定之電流值之值之前,僅進行基於濺鍍氣體之預濺鍍,將附著於靶材60之表面之初始氧化覆膜充分地濺鍍去除(步驟S150)。 Next, before the sputtering current value monitored by the control unit 200 becomes a value lower than the specific current value, only the pre-sputtering by the sputtering gas is performed, and the initial oxide film adhering to the surface of the target 60 is sufficiently Sputtering is removed (step S150).

若充分地去除靶材60之表面之初始氧化覆膜,則濺鍍電流值以較低之值成為大致固定值,因而此時來自反應性氣體供給部191之氧氣之反應性氣體(更準確而言,較理想為5%之氧氣與Ar等惰性氣體之稀釋混合氣體)之供給經由流量控制器192、電漿產生氣體導入部19而開始(步驟S160,圖5之時間t4)。再者,於開始反應性氣體之供給之後,處理室113之壓力仍維持為目標壓力。又,就濺鍍之性質而言,於開始反應性氣體之供給之後,濺鍍電流值亦於短時間內下降。 When the initial oxide film on the surface of the target 60 is sufficiently removed, the sputtering current value becomes a substantially constant value at a low value, and thus the reactive gas of oxygen from the reactive gas supply portion 191 at this time (more accurate) In other words, the supply of the 5% oxygen and the diluted mixed gas of the inert gas such as Ar) is started via the flow rate controller 192 and the plasma generated gas introduction unit 19 (step S160, time t4 in FIG. 5). Further, after the supply of the reactive gas is started, the pressure of the processing chamber 113 is maintained at the target pressure. Further, in terms of the nature of the sputtering, the sputtering current value also drops in a short time after the supply of the reactive gas is started.

繼而,逐漸增加開始供給之反應性氣體之導入量,將濺鍍電流值暫時提高至目標電流值以上。其後,此次逐漸減少反應性氣體之導入量,並降低濺鍍電流值,於濺鍍電流值達到目標電流值時,打開成膜擋板,開始對基板74之表面之氧化鋁之成膜處理,並且以濺鍍電流值維持為目標電流值之方式,開始控制反應性氣體之導入量(步驟S170,圖5之時間t5)。再者,圖5之實驗結果中,自時間t3至時間t5之經過時間為5分鐘。 Then, the introduction amount of the reactive gas to be supplied is gradually increased, and the sputtering current value is temporarily increased to be equal to or higher than the target current value. Thereafter, the introduction amount of the reactive gas is gradually reduced, and the sputtering current value is lowered. When the sputtering current value reaches the target current value, the film forming baffle is opened to start the film formation of the aluminum oxide on the surface of the substrate 74. The treatment is started, and the introduction amount of the reactive gas is started to be controlled so that the sputtering current value is maintained as the target current value (step S170, time t5 of FIG. 5). Further, in the experimental results of Fig. 5, the elapsed time from time t3 to time t5 was 5 minutes.

於開始成膜處理之後,仍繼續反應性氣體之導入量之控制,而將濺鍍電流值維持為目標電流值。再者,圖5所示之實驗結果中,反應性氣體之導入量以曲線L11為基準反覆增減,並且隨著時間之經過而逐漸增加。其係由如下干擾因素所致,即,例如附著並殘留於基板74之水分等於電漿產生時瞬間分解,氧氣(反應性氣體)急遽增加,自隨著進行成膜處理而殘留之水分所產生之反應性氣體減少。以濺鍍電流值達到目標電流值之方式控制自反應性氣體供給部191供給之反應性氣體之導入量之結果為,該導入量逐漸增加。於該導入量之控制中,亦可根據反應性氣體之電漿發光強度之變化而預測濺鍍電流值之 變化,以濺鍍電流值達到目標電流值之方式,控制反應性氣體之導入量。藉此,將濺鍍電流值保持為目標電流值之精度得以進一步提高。 After the film formation process is started, the control of the introduction amount of the reactive gas is continued, and the sputtering current value is maintained at the target current value. Further, in the experimental results shown in Fig. 5, the introduction amount of the reactive gas was repeatedly increased or decreased based on the curve L11, and gradually increased with the passage of time. It is caused by the following interference factors, that is, for example, the moisture attached to and remaining on the substrate 74 is equal to the instantaneous decomposition of the plasma, the oxygen (reactive gas) is rapidly increased, and the residual moisture is generated from the film formation process. The reactive gas is reduced. As a result of controlling the introduction amount of the reactive gas supplied from the reactive gas supply unit 191 so that the sputtering current value reaches the target current value, the introduction amount is gradually increased. In the control of the introduction amount, the sputtering current value can also be predicted according to the change of the plasma luminous intensity of the reactive gas. The change is to control the introduction amount of the reactive gas in such a manner that the sputtering current value reaches the target current value. Thereby, the accuracy of maintaining the sputtering current value as the target current value is further improved.

圖8係模式性地表示濺鍍電流值與反應性氣體之電漿發光強度間之關係之圖。圖9係模式性地表示使用濺鍍電流值之變化之預測的反應性氣體之導入量(氧氣供給量)之控制例之圖。 Fig. 8 is a view schematically showing the relationship between the sputtering current value and the plasma luminous intensity of the reactive gas. FIG. 9 is a view schematically showing an example of control of the introduction amount (oxygen supply amount) of the reactive gas using the predicted change in the sputtering current value.

如上所述,濺鍍電流值係與靶材60表面之鋁之氧化度相應之電流值,因氧化反應之性質所致之時間延遲,而使濺鍍電流值相對於處理室113內之氧氣之反應性氣體之電漿發光強度之變化而延遲變化。具體而言,在相對於目標電流值Ia,例如濺鍍電流如曲線51般變化之情形時,反應性氣體之電漿發光強度例如如曲線52所示般變化。如此,反應性氣體之電漿發光強度根據濺鍍電流值之變化而於時間上早於濺鍍電流值進行變化。 As described above, the sputtering current value is a current value corresponding to the degree of oxidation of aluminum on the surface of the target 60, and the time delay due to the nature of the oxidation reaction causes the sputtering current value to be relative to the oxygen in the processing chamber 113. The change in the luminous intensity of the plasma of the reactive gas is delayed. Specifically, when the sputtering current changes as the curve 51 with respect to the target current value Ia, for example, the plasma luminous intensity of the reactive gas changes as shown by the curve 52, for example. Thus, the plasma luminous intensity of the reactive gas changes temporally earlier than the sputtering current value according to the change in the sputtering current value.

圖9中,於及至時間T21之氧氣之反應性氣體導入至處理室113之導入量(氧氣供給量)如曲線55所示般控制為固定值之情形時,相對於目標電流值Ia,濺鍍電流值由曲線53表示,反應性氣體之電漿發光強度由曲線54表示。時間T21係獲得實驗中最新資料之時間。於該情形時,於時間T21即將到來之前之期間,反應性氣體之電漿發光強度變小,因此可預測到於時間T21以後,隨著時間之經過,濺鍍電流值亦例如圖9中虛線所示般變小。於該情形時,於時間T21以後,濺鍍電流值實際地變化之前,藉由使反應性氣體之導入量例如曲線55之虛線所示之部分般增加,而可使濺鍍電流值之與目標電流值Ia之偏差更小。因此,可使所要成膜之氧化鋁之氧化度更穩定且使氧化鋁成膜於基板74。再者,由於為透過窗部17之光,故而藉由分光器111所檢測之反應性氣體之電漿發光強度存在因窗部17之污垢而使分光器111所檢測之電漿發光強度之絕對值產生偏差之情形,為了使電漿發光強度之變化之方向變正確,較佳為基於該變化之方向而控制反應性氣體之導入 量。 In Fig. 9, when the introduction amount (oxygen supply amount) of the oxygen-reactive gas introduced into the processing chamber 113 at the time T21 is controlled to a fixed value as shown by the curve 55, the sputtering is performed with respect to the target current value Ia. The current value is represented by curve 53, and the plasma luminescence intensity of the reactive gas is indicated by curve 54. Time T21 is the time to obtain the most up-to-date information in the experiment. In this case, the plasma luminescence intensity of the reactive gas becomes small during the period immediately before the time T21, so it can be predicted that after the time T21, the sputtering current value is also, for example, the dotted line in FIG. 9 after the lapse of time. As shown, it becomes smaller. In this case, after the time T21, before the sputtering current value actually changes, the sputtering current value and the target can be made by increasing the introduction amount of the reactive gas such as the portion indicated by the broken line of the curve 55. The deviation of the current value Ia is smaller. Therefore, the degree of oxidation of the alumina to be film-formed can be made more stable and the alumina can be formed on the substrate 74. Further, since the light is transmitted through the window portion 17, the plasma luminous intensity of the reactive gas detected by the spectroscope 111 has an absolute intensity of the plasma light detected by the spectroscope 111 due to the dirt of the window portion 17. In the case where the value is deviated, in order to change the direction of the change in the luminous intensity of the plasma, it is preferable to control the introduction of the reactive gas based on the direction of the change. the amount.

返回至圖7,若經成膜之氧化鋁之膜厚達到特定厚度(或者經過特定時間),則關閉成膜擋板,結束成膜處理(步驟S180,圖5之時間t6)。再者,圖5之實驗結果中,自時間t5至時間t6之經過時間為20分鐘。繼而,停止利用濺鍍用電源162對底板14施加濺鍍電壓(偏壓)(步驟S190,圖5之時間t7),於該停止後(或與停止同時),停止自高頻電源161向高頻天線80供給高頻電力(步驟S200,圖5之時間t8)。其次,停止氣體之供給(步驟S210,圖5之時間t9),打開閘極351,將基板74自腔室11之處理室113中搬出(步驟S220)。 Returning to Fig. 7, when the film thickness of the film-formed alumina reaches a specific thickness (or a specific time elapses), the film formation baffle is closed, and the film formation process is terminated (step S180, time t6 of Fig. 5). Further, in the experimental results of Fig. 5, the elapsed time from time t5 to time t6 was 20 minutes. Then, the sputtering voltage (bias) is applied to the substrate 14 by the sputtering power source 162 (step S190, time t7 of FIG. 5), and after the stop (or at the same time as the stop), the high frequency power supply 161 is stopped. The frequency antenna 80 supplies high frequency power (step S200, time t8 of Fig. 5). Next, the supply of the gas is stopped (step S210, time t9 in Fig. 5), the gate 351 is opened, and the substrate 74 is carried out from the processing chamber 113 of the chamber 11 (step S220).

根據如上之本實施形態之氧化鋁之成膜方法,第1電漿產生步驟係使用設置於導入有濺鍍氣體及氧氣之反應性氣體之腔室11內且包含卷數未達一圈之導體之高頻天線80,至少於第2電漿產生步驟中於腔室11內產生高頻電感耦合電漿。而且,第2電漿產生步驟係對靶材60施加濺鍍電壓而產生磁控電漿。因此,藉由氧自由基之增加、成膜對象之基板74上之氧化反應之促進、以及伴隨其等而產生之已氧化之靶材60表面之軟化之綜合性效果,而使成膜速度高速化。又,根據本發明,於第2電漿產生步驟中將濺鍍電壓進行定電壓控制,並且以流動於磁控陰極之濺鍍電流值達到目標電流值之方式,控制第2電漿產生步驟中反應性氣體之導入量。於將濺鍍電壓進行定電壓控制之情形時,即以電壓固定模式驅動濺鍍電源之情形時,形成於基板74上之氧化鋁膜之氧化度穩定於與腔室11內之氧氣量、即反應性氣體量相應之穩定之平衡點。又,於將濺鍍電壓進行定電壓控制之情形時,鋁靶60表面之氧化度越高,即腔室11內之反應性氣體量越多,則濺鍍電流值變得越大,並且成膜於基板74上之氧化鋁之氧化度亦會變得越高。因此,根據本發明,藉由以濺鍍電流值達到目標電流值之方式將反應性氣體導入至腔室11內,無關例如由於吸附於基板74之水分等而產生之 反應性氣體等干擾因素,而可使形成於基板74上之氧化鋁膜之氧化度穩定。即,可使氧化度穩定地、且以較快之成膜速度成膜氧化鋁。 According to the film forming method of alumina according to the embodiment of the present invention, the first plasma generating step uses a conductor provided in the chamber 11 into which the reactive gas of the sputtering gas and the oxygen gas is introduced and which includes the number of coils less than one turn. The high frequency antenna 80 generates high frequency inductively coupled plasma in the chamber 11 at least in the second plasma generating step. Further, the second plasma generating step applies a sputtering voltage to the target 60 to generate a magnetron plasma. Therefore, the film formation speed is high by the increase in oxygen radicals, the promotion of the oxidation reaction on the substrate 74 of the film formation target, and the softening effect of the surface of the oxidized target 60 generated by the oxidation target 60. Chemical. Further, according to the present invention, the sputtering voltage is subjected to constant voltage control in the second plasma generating step, and the second plasma generating step is controlled in such a manner that the sputtering current value flowing through the magnetron cathode reaches the target current value. The amount of introduction of reactive gas. When the sputtering voltage is controlled by constant voltage, that is, when the sputtering power source is driven in the voltage fixed mode, the degree of oxidation of the aluminum oxide film formed on the substrate 74 is stabilized by the amount of oxygen in the chamber 11, that is, The amount of reactive gas corresponds to a stable equilibrium point. Further, in the case where the sputtering voltage is subjected to constant voltage control, the higher the degree of oxidation of the surface of the aluminum target 60, that is, the larger the amount of reactive gas in the chamber 11, the larger the sputtering current value becomes, and The degree of oxidation of the alumina of the film on the substrate 74 also becomes higher. Therefore, according to the present invention, the reactive gas is introduced into the chamber 11 by the sputtering current value reaching the target current value irrespective of, for example, moisture adsorbed on the substrate 74 or the like. The degree of oxidation of the aluminum oxide film formed on the substrate 74 can be stabilized by an interference factor such as a reactive gas. That is, the alumina can be formed stably at a relatively high film formation rate.

又,根據如上所述之本實施形態之氧化鋁之成膜方法,目標電流值為所要成膜之氧化鋁之氧化度成為如下氧化度時之濺鍍電流值,即化學計量之氧化鋁與氧化度較化學計量之氧化鋁低之氧化鋁各自之氧化度之邊界附近的氧化度。該氧化度為所要成膜之氧化鋁之鈍化效果變高之氧化度,並且亦為成膜速度較快之氧化度。因此,能夠以較快之成膜速度穩定地成膜適於p型矽基板之鈍化膜並發揮較佳之鈍化效果之氧化鋁。 Further, according to the film forming method of alumina according to the present embodiment as described above, the target current value is a sputtering current value when the degree of oxidation of the alumina to be formed is the following oxidation degree, that is, stoichiometric alumina and oxidation. The degree of oxidation near the boundary of the oxidation degree of each of the aluminas having a lower stoichiometric amount of alumina. The degree of oxidation is an oxidation degree at which the passivation effect of the alumina to be film-formed becomes high, and is also a degree of oxidation at a faster film formation rate. Therefore, alumina which is suitable for a passivation film of a p-type germanium substrate and exhibits a preferable passivation effect can be stably formed at a relatively fast film formation speed.

又,根據如上所述之本實施形態之氧化鋁之成膜方法,於控制步驟中,根據先於實際之濺鍍電流值之變化而對應於該變化發生變化的反應性氣體之電漿之發光強度之變化,預測濺鍍電流值之變化,以濺鍍電流值達到目標電流值之方式,控制反應性氣體之導入量。因此,可使氧化度更穩定並成膜氧化鋁。 Further, according to the method for forming a film of alumina according to the present embodiment as described above, in the control step, the light of the plasma corresponding to the reactive gas which changes in response to the change in the actual sputtering current value is used. The change in intensity predicts the change in the value of the sputtering current, and controls the amount of introduction of the reactive gas in such a manner that the sputtering current value reaches the target current value. Therefore, the degree of oxidation can be made more stable and the alumina can be formed.

又,根據如上所述之本實施形態之氧化鋁之成膜方法,濺鍍電壓為負電壓。因此,可進而抑制界面之損傷,並且可於基板74上成膜氧化鋁,從而成膜較太陽電池矽基板之鈍化膜更佳之氧化鋁。 Moreover, according to the film forming method of the alumina of this embodiment as described above, the sputtering voltage is a negative voltage. Therefore, damage to the interface can be further suppressed, and alumina can be formed on the substrate 74 to form a better alumina than the passivation film of the solar cell ruthenium substrate.

已詳細表示並記載本發明,但上述記載於所有態樣中為例示而並不限定於該等態樣。因此,本發明可於其發明之範圍內將實施形態適當變化、省略。例如為提高維護性能,高頻天線係可不將其U形狀之中央部分之直線部分自天線固定塊182突設地配置,又,自維護性與電漿之產生能力之平衡來判斷,亦可以僅突設其直線部分之上側半部分之方式配置。又,於對複數個基板74連續進行成膜之情形時,亦可卸除腔室11之上部壁面,在將分別安裝有基板74之複數個基板平台15以於腔室11之上部不出現間隙之方式使鄰接之基板平台15彼此之前端與後端對接並沿著搬送方向排列之狀態下,搬送各基板平台15,進 行對各基板74之成膜處理。於該情形時,於利用預濺鍍進行靶材60之初始氧化覆膜之去除時,例如,藉由將複數個基板平台15中之最前端之基板平台15作為未安裝有基板74之虛設基板,可不使用成膜擋板而去除初始氧化覆膜。 The present invention has been described and illustrated in detail, but the description above is exemplified in all aspects and is not limited to the aspects. Therefore, the present invention can be appropriately changed or omitted within the scope of the invention. For example, in order to improve the maintenance performance, the high-frequency antenna may not be arranged such that the straight portion of the central portion of the U shape is protruded from the antenna fixing block 182, and the balance between the self-maintenance and the ability to generate plasma may be determined. Arranged in such a manner that the upper half of the straight portion is protruded. Further, when a plurality of substrates 74 are continuously formed into a film, the upper wall surface of the chamber 11 may be removed, and a plurality of substrate stages 15 on which the substrate 74 are attached may be provided so that no gap is formed in the upper portion of the chamber 11. In a manner that the adjacent substrate platforms 15 are butted against each other at the front end and the rear end, and are arranged in the transport direction, the substrate platforms 15 are transported. The film formation process for each of the substrates 74 is performed. In this case, when the initial oxide film of the target 60 is removed by pre-sputtering, for example, by using the substrate stage 15 at the foremost end among the plurality of substrate stages 15 as a dummy substrate on which the substrate 74 is not mounted. The initial oxide film can be removed without using a film forming baffle.

10‧‧‧濺鍍裝置 10‧‧‧ Sputtering device

11‧‧‧腔室 11‧‧‧ chamber

12‧‧‧磁控濺鍍用磁鐵 12‧‧‧ Magnets for magnetron sputtering

14‧‧‧底板(陰極) 14‧‧‧Bottom plate (cathode)

15‧‧‧基板平台 15‧‧‧Substrate platform

17‧‧‧窗部 17‧‧‧ Window Department

18‧‧‧靶材.天線配置部 18‧‧‧ Targets. Antenna configuration department

19‧‧‧電漿產生氣體導入部 19‧‧‧ Plasma generation gas introduction

20‧‧‧氣體導入口 20‧‧‧ gas inlet

24‧‧‧靶材保持部 24‧‧‧ Target Holding Department

60‧‧‧靶材(鋁靶) 60‧‧‧ Target (aluminum target)

74‧‧‧基板 74‧‧‧Substrate

80‧‧‧高頻天線 80‧‧‧High frequency antenna

90‧‧‧電漿產生部 90‧‧‧The Plasma Generation Department

111‧‧‧分光器 111‧‧‧ Spectroscope

112‧‧‧探針 112‧‧‧Probe

113‧‧‧處理室 113‧‧‧Processing room

151‧‧‧冷媒 151‧‧‧Refrigerant

161‧‧‧高頻電源 161‧‧‧High frequency power supply

162‧‧‧濺鍍用電源 162‧‧‧Power supply for sputtering

163‧‧‧匹配電路 163‧‧‧Matching circuit

164‧‧‧電流計 164‧‧‧ galvanometer

181‧‧‧靶材配置塊 181‧‧‧target configuration block

182‧‧‧天線固定塊 182‧‧‧Antenna fixed block

189‧‧‧陽極 189‧‧‧Anode

191‧‧‧反應性氣體供給部 191‧‧‧Reactive Gas Supply Department

192‧‧‧流量控制器 192‧‧‧Flow Controller

200‧‧‧控制部 200‧‧‧Control Department

351‧‧‧閘極 351‧‧‧ gate

411‧‧‧保護管 411‧‧‧Protection tube

X‧‧‧軸 X‧‧‧ axis

Y‧‧‧軸 Y‧‧‧ axis

Z‧‧‧軸 Z‧‧‧ axis

Claims (9)

一種氧化鋁之成膜方法,其係於設置有形成靜磁場之磁控陰極之真空容器中,將濺鍍氣體及氧氣之反應性氣體以該真空容器內之壓力達到目標壓力之方式進行控制並導入,對設置於該陰極之鋁靶進行濺鍍,於與該鋁靶對向之矽基板上形成氧化膜;且包括以下步驟:第1電漿產生步驟,其係於導入有上述濺鍍氣體及上述反應性氣體之真空容器內產生電漿;第2電漿產生步驟,其係對上述鋁靶施加負電壓、包含負電壓及正電壓之直流脈衝、及交流之任一種濺鍍電壓,藉由上述靜磁場而產生磁控電漿;及控制步驟,其控制導入至上述真空容器內之上述反應性氣體之導入量;且上述第2電漿產生步驟係將上述濺鍍電壓進行定電壓控制之步驟;上述控制步驟係以流動於上述磁控陰極之濺鍍電流值達到目標電流值之方式,控制上述第2電漿產生步驟中上述反應性氣體之導入量之步驟;上述第1電漿產生步驟係使用設置於上述真空容器內且包含卷數未達一圈之導體之高頻天線,至少於上述第2電漿產生步驟中產生高頻電感耦合電漿之步驟。 A method for forming a film of alumina, which is controlled in a vacuum vessel provided with a magnetron cathode for forming a static magnetic field, and controls a sputtering gas and a reactive gas of oxygen to a target pressure in a state in which the pressure in the vacuum vessel reaches a target pressure Introducing, sputtering an aluminum target disposed on the cathode, forming an oxide film on the substrate opposite to the aluminum target; and comprising the steps of: a first plasma generating step of introducing the sputtering gas And a plasma generated in the vacuum vessel of the reactive gas; and a second plasma generating step of applying a negative voltage, a DC pulse including a negative voltage and a positive voltage, and a sputtering voltage to the aluminum target, Generating a magnetron plasma by the static magnetic field; and controlling a step of controlling an introduction amount of the reactive gas introduced into the vacuum vessel; and the second plasma generating step is to perform constant voltage control on the sputtering voltage a step of controlling the reactive gas in the second plasma generating step by a method in which a sputtering current value flowing through the magnetron cathode reaches a target current value a step of introducing the amount of the first plasma generation step by using a high frequency antenna provided in the vacuum container and including a conductor having a number of windings less than one turn, and generating a high frequency inductor at least in the second plasma generating step The step of coupling the plasma. 如請求項1之氧化鋁之成膜方法,其中上述目標電流值係所成膜之氧化鋁之氧化度成為化學計量之氧化鋁與氧化度較化學計量之氧化鋁低之氧化鋁各自之氧化度之邊界附近的氧化度時之上述濺鍍電流值。 The method of forming a film of alumina according to claim 1, wherein the target current value is a degree of oxidation of the alumina of the film formed into a stoichiometric amount of alumina and a degree of oxidation of the alumina having a lower oxidation degree than the stoichiometric amount of alumina. The above-mentioned sputtering current value at the time of oxidation near the boundary. 如請求項1或2之氧化鋁之成膜方法,其中上述控制步驟係根據上述反應性氣體之電漿之發光強度之變化而預測上述濺鍍電流值之變化,以上述濺鍍電流值達到上述目標電流值之方式,控制上述反應性氣體之導入量。 The method for forming a film of alumina according to claim 1 or 2, wherein the controlling step predicts a change in the sputtering current value according to a change in the luminous intensity of the plasma of the reactive gas, and the sputtering current value is as described above. The amount of the target current value is controlled to control the introduction amount of the above reactive gas. 如請求項1或2之氧化鋁之成膜方法,其中上述濺鍍電壓為負電壓。 A method of forming a film of alumina according to claim 1 or 2, wherein said sputtering voltage is a negative voltage. 如請求項1或2之氧化鋁之成膜方法,其中上述目標壓力為0.2Pa以上且7Pa以下。 The method of forming a film of alumina according to claim 1 or 2, wherein the target pressure is 0.2 Pa or more and 7 Pa or less. 如請求項5之氧化鋁之成膜方法,其中上述目標壓力為0.4Pa以上且2Pa以下。 The method of forming a film of alumina according to claim 5, wherein the target pressure is 0.4 Pa or more and 2 Pa or less. 如請求項1或2之氧化鋁之成膜方法,其中上述濺鍍電壓之負電壓之絕對值為100V以上且300V以下。 The method for forming a film of alumina according to claim 1 or 2, wherein the absolute value of the negative voltage of the sputtering voltage is 100 V or more and 300 V or less. 如請求項7之氧化鋁之成膜方法,其中上述濺鍍電壓之負電壓之絕對值為150V以上且250V以下。 The method of forming a film of alumina according to claim 7, wherein the absolute value of the negative voltage of the sputtering voltage is 150 V or more and 250 V or less. 一種濺鍍裝置,其係於設置有形成靜磁場之磁控陰極之真空容器中,將濺鍍氣體及氧氣之反應性氣體以該真空容器內之壓力達到目標壓力之方式進行控制並導入,對設置於該陰極之鋁靶進行濺鍍,於與該鋁靶對向之矽基板上形成氧化膜;且包括如下構件:電漿產生氣體導入部,其將上述濺鍍氣體及上述反應性氣體導入至上述真空容器內;控制部,其控制藉由上述電漿產生氣體導入部導入至上述處理空間之上述反應性氣體之導入量;高頻天線,其設置於上述真空容器內且包含卷數未達一圈之導體;高頻電源,其對上述高頻天線供給高頻電力,以使得於導入 有上述濺鍍氣體及上述反應性氣體之上述真空容器內產生高頻電感耦合電漿;及濺鍍用電源,其對上述鋁靶施加負電壓、包含負電壓及正電壓之直流脈衝、及交流之任一種濺鍍電壓,以使得藉由上述磁控陰極所形成之靜磁場而於導入有上述濺鍍氣體及上述反應性氣體之上述真空容器內產生磁控電漿;且上述濺鍍用電源將上述濺鍍電壓進行定電壓控制;上述控制部係以流動於上述磁控陰極之濺鍍電流值達到目標電流值之方式,控制於上述磁控電漿之產生過程中上述電漿產生氣體導入部導入至上述真空容器內之上述反應性氣體之導入量。 A sputtering apparatus is provided in a vacuum vessel provided with a magnetron cathode for forming a static magnetic field, and the reactive gas of the sputtering gas and the oxygen gas is controlled and introduced in such a manner that the pressure in the vacuum vessel reaches a target pressure. An aluminum target disposed on the cathode is sputtered to form an oxide film on the substrate opposite to the aluminum target; and includes a member: a plasma generating gas introduction portion that introduces the sputtering gas and the reactive gas a control unit that controls an introduction amount of the reactive gas introduced into the processing space by the plasma generating gas introduction unit, and a high frequency antenna provided in the vacuum container and including a number of volumes a conductor of one turn; a high frequency power supply that supplies high frequency power to the above high frequency antenna to enable introduction a high-frequency inductively coupled plasma is generated in the vacuum container having the sputtering gas and the reactive gas; and a power source for sputtering, which applies a negative voltage to the aluminum target, a DC pulse including a negative voltage and a positive voltage, and an alternating current Any one of a sputtering voltage such that a magnetron is generated in the vacuum vessel into which the sputtering gas and the reactive gas are introduced by a static magnetic field formed by the magnetron; and the sputtering power source Performing constant voltage control on the sputtering voltage; the control unit controls the plasma generation gas introduction during the generation of the magnetron plasma by the sputtering current value flowing through the magnetron cathode reaching a target current value The amount of introduction of the above-mentioned reactive gas introduced into the vacuum container.
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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI696719B (en) * 2018-01-25 2020-06-21 日商斯庫林集團股份有限公司 Film forming apparatus and film forming method
US11306392B2 (en) 2016-06-07 2022-04-19 Nitto Denko Corporation Method for producing optical film
TWI764904B (en) * 2016-06-07 2022-05-21 日商日東電工股份有限公司 Manufacturing method of optical film

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6264248B2 (en) * 2014-09-26 2018-01-24 日新電機株式会社 Film forming method and sputtering apparatus
JP6670546B2 (en) * 2015-02-17 2020-03-25 日東電工株式会社 Thin film deposition method
CN107406967B (en) * 2015-03-10 2019-03-05 株式会社爱发科 The film build method and forming method and sputtering equipment of pellumina
JP6775972B2 (en) * 2016-03-17 2020-10-28 芝浦メカトロニクス株式会社 Film formation equipment and film formation method
JP6916699B2 (en) * 2017-09-14 2021-08-11 株式会社Screenホールディングス Film formation method and film deposition equipment
JP6942015B2 (en) * 2017-09-27 2021-09-29 株式会社Screenホールディングス Film formation equipment and film formation method
JP2021066895A (en) * 2018-02-26 2021-04-30 株式会社アルバック Film deposition method
US11384421B2 (en) 2018-03-16 2022-07-12 The Government Of The United States Of America, As Represented By The Secretary Of The Navy High temperature sputtered stoichiometric amorphous aluminum oxide

Family Cites Families (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE4106770C2 (en) * 1991-03-04 1996-10-17 Leybold Ag Performing reactive coating of a substrate
JP3689524B2 (en) * 1996-03-22 2005-08-31 キヤノン株式会社 Aluminum oxide film and method for forming the same
JP4531145B2 (en) * 1997-05-27 2010-08-25 株式会社アルバック Ultra-thin insulating film formation method
EP1015654A1 (en) * 1997-09-16 2000-07-05 Fraunhofer-Gesellschaft Zur Förderung Der Angewandten Forschung E.V. METHOD FOR COATING SUBSTRATES WITH ALUMINUM OXIDE (Al 2?O 3?) AND COATING A WORK PIECE USING SAID METHOD
JP3866615B2 (en) * 2002-05-29 2007-01-10 株式会社神戸製鋼所 Reactive sputtering method and apparatus
WO2005093797A1 (en) * 2004-03-26 2005-10-06 Nissin Electric Co., Ltd. Method and equipment for forming crystalline silicon thin film
JP4720298B2 (en) * 2005-06-07 2011-07-13 株式会社ブリヂストン Method for forming conductive compound thin film
JP2007031815A (en) * 2005-07-29 2007-02-08 Shimadzu Corp Planar magnetron sputtering apparatus and planar magnetron sputtering film forming method
JP2009287088A (en) * 2008-05-29 2009-12-10 Fujifilm Corp Film deposition apparatus, film deposition method and barrier film
CN102144044B (en) * 2008-08-28 2015-11-25 Emd株式会社 Thin film-forming sputtering device
JP5475506B2 (en) * 2010-02-26 2014-04-16 株式会社イー・エム・ディー Sputtering thin film forming equipment
EP2752501A4 (en) * 2011-08-30 2015-02-18 Emd Corp Sputtering thin film forming apparatus

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US11306392B2 (en) 2016-06-07 2022-04-19 Nitto Denko Corporation Method for producing optical film
TWI764904B (en) * 2016-06-07 2022-05-21 日商日東電工股份有限公司 Manufacturing method of optical film
TWI696719B (en) * 2018-01-25 2020-06-21 日商斯庫林集團股份有限公司 Film forming apparatus and film forming method

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TWI504773B (en) 2015-10-21
JP2014189827A (en) 2014-10-06

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