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CN102906301B - Ito sputtering target - Google Patents

Ito sputtering target Download PDF

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Publication number
CN102906301B
CN102906301B CN201180025334.9A CN201180025334A CN102906301B CN 102906301 B CN102906301 B CN 102906301B CN 201180025334 A CN201180025334 A CN 201180025334A CN 102906301 B CN102906301 B CN 102906301B
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ito
target
indium
film
targets
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CN102906301A (en
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挂野崇
铃木了
栗原敏也
中村祐一郎
关和广
牧野修仁
熊原吉一
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JX Nippon Mining and Metals Corp
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    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
    • C23C14/3464Sputtering using more than one target
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/06Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the coating material
    • C23C14/08Oxides
    • C23C14/086Oxides of zinc, germanium, cadmium, indium, tin, thallium or bismuth
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
    • C23C14/3407Cathode assembly for sputtering apparatus, e.g. Target

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

Abstract

The present invention relates to an ITO sputtering target which is configured by arranging a plurality of ITO divided targets on a backing plate and bonding the ITO divided targets to the backing plate, wherein a coating layer of one substance selected from indium, an indium alloy and a tin alloy is provided only on the side surface on the side of a gap between the arranged ITO divided targets. The subject of the invention is to provide: even in the continuous sputtering of the divided ITO target, the ITO sputtering target, especially the sputtering target for FPD, can suppress the generation of nodules and abnormal discharge, and can obtain a film with high uniformity of film characteristics, wherein the characteristics of the film formed on the substrate opposite to the gap part are not different from those of the film at other parts.

Description

ITO溅射靶ITO sputtering target

技术领域technical field

本发明涉及通过溅射法制作透明导电膜时使用的溅射靶,特别涉及包含多片靶材,具有分割部的ITO溅射靶。The present invention relates to a sputtering target used when producing a transparent conductive film by a sputtering method, and particularly relates to an ITO sputtering target including a plurality of target materials and having a divided part.

背景技术Background technique

透明导电膜形成用ITO薄膜,作为以液晶显示器、触控面板、EL显示器等为代表的显示装置的透明电极广泛使用。多数情况下,ITO等透明导电膜形成用氧化物薄膜是通过溅射形成的。ITO thin films for forming transparent conductive films are widely used as transparent electrodes of display devices such as liquid crystal displays, touch panels, and EL displays. Oxide thin films for forming transparent conductive films such as ITO are often formed by sputtering.

ITO(铟锡氧化物)薄膜,具有高导电率、高透射率的特性,因此用于平板用显示电极等。近年来,伴随平板显示器(FPD)的大型化,对于ITO靶的大型化要求也日渐增强。ITO (Indium Tin Oxide) thin film has high conductivity and high transmittance, so it is used in display electrodes for flat panels, etc. In recent years, along with the increase in the size of the flat panel display (FPD), the demand for the increase in the size of the ITO target is also increasing.

但是,由于用于制作大型ITO的新型设备投资以及翘曲等引起的成品率下降,ITO的大型化非常困难。因此,目前大型ITO靶使用的是将多个小型ITO构件接合而形成的多分割靶。However, it is very difficult to increase the size of ITO due to investment in new equipment for producing large ITO and reduction in yield due to warpage and the like. Therefore, currently, a large-sized ITO target uses a multi-segmented target formed by bonding a plurality of small-sized ITO members.

使用前述的多分割靶长时间进行溅射时,已知在靶的表面、特别是分割部部分析出称为结瘤的被认为是铟的低氧化物的黑色附着物,容易引起异常放电,并且成为薄膜表面的粉粒产生源。When sputtering is performed for a long time using the above-mentioned multi-segmented target, it is known that black deposits called nodules, which are considered to be indium suboxides, are deposited on the surface of the target, especially at the segmented parts, and abnormal discharges are likely to occur. And it becomes the source of particle generation on the surface of the film.

对此,在现有技术中,记载了通过在整个空隙部分埋入铟或各种合金的方法可以抑制溅射时产生结瘤和异常放电。On the other hand, in the prior art, it is described that the generation of nodules and abnormal discharge during sputtering can be suppressed by embedding indium or various alloys in the entire void.

例如,在专利文献1中,公开了在空隙部分填充与靶主体的铟锡原子数比相等的铟-锡合金的方法。但是,为此,需要测定靶主体的铟锡原子数比,每次都需要基于该结果调节填充的铟-锡合金组成,因此靶的生产率存在问题。For example, Patent Document 1 discloses a method of filling voids with an indium-tin alloy having an atomic number ratio of indium tin of the target main body. However, for this purpose, it is necessary to measure the indium-tin atomic ratio of the target body, and it is necessary to adjust the composition of the indium-tin alloy to be filled based on the result every time, so there is a problem in the productivity of the target.

另外,由于将铟-锡合金注入整个间隙部分,因此存在由其上部形成的膜的电特性与由其它部分形成的膜的电特性不同的问题。In addition, since the indium-tin alloy is injected into the entire gap portion, there is a problem that the electrical characteristics of the film formed from the upper portion thereof are different from those of the film formed from other portions.

另外,在专利文献2中,公开了在空隙部分填充铟的方法,在专利文献3中,公开了在空隙部分填充具有比接合材料高的熔点的合金的方法。Also, Patent Document 2 discloses a method of filling indium in the void, and Patent Document 3 discloses a method of filling the void with an alloy having a melting point higher than that of the joining material.

但是,这些方法中,由于将铟注入整个空隙部分,因此存在由其上部形成的膜的电特性与由其它部分形成的膜的电特性不同的问题。However, in these methods, since indium is injected into the entire void portion, there is a problem that the electrical characteristics of the film formed above it are different from those of the film formed in other portions.

在专利文献4中,公开了在空隙部分中填充虽然构成元素与金属氧化物烧结体相同但是组成不同的材料的方法。但是,氧量少的情况下,由于具有与通常的合金基本相同的特性,因此存在由其上部形成的膜的电特性与由其它部分形成的膜的电特性不同的问题,另外,相反地,氧量多的情况下,由于特性与ITO基本相同,因此存在不能在低温下熔融注入空隙部分的问题。Patent Document 4 discloses a method of filling voids with a material having the same constituent elements as the metal oxide sintered body but having a different composition. However, when the amount of oxygen is small, since it has substantially the same characteristics as a general alloy, there is a problem that the electrical characteristics of the film formed on its upper part are different from those of the film formed by other parts. In addition, conversely, When there is a large amount of oxygen, since the characteristics are basically the same as those of ITO, there is a problem that it cannot be melted and injected into the void at low temperature.

现有技术文献prior art literature

专利文献patent documents

专利文献1:日本特开平01-230768号公报Patent Document 1: Japanese Patent Application Laid-Open No. 01-230768

专利文献2:日本特开平08-144052号公报Patent Document 2: Japanese Patent Application Laid-Open No. 08-144052

专利文献3:日本特开2000-144400号公报Patent Document 3: Japanese Patent Laid-Open No. 2000-144400

专利文献4:日本特开2010-106330号公报Patent Document 4: Japanese Patent Laid-Open No. 2010-106330

发明内容Contents of the invention

本发明的课题在于提供:即使在分割ITO靶的连续溅射时,也可以抑制结瘤的产生和异常放电,并且可以得到在与空隙部分相对的衬底上形成的膜的特性与其它部分的膜的特性无差异,即膜特性的均匀性高的膜的ITO溅射靶,特别是FPD用溅射靶。The object of the present invention is to provide: even in the continuous sputtering of the divided ITO target, the generation of nodules and abnormal discharge can be suppressed, and the characteristics of the film formed on the substrate opposite to the void portion can be compared with those of other portions. There is no difference in film properties, that is, an ITO sputtering target of a film with high uniformity of film properties, especially a sputtering target for FPD.

为了解决上述课题,本发明人进行了广泛深入的研究,结果发现,通过由多个分割靶构成ITO溅射靶,并且对该多个分割靶的边缘部进行设计,能够提供可以通过排列分割靶而制作大型的靶,可以减少由各分割靶的边缘部引起的粉粒的产生导致的不良的溅射靶,特别是FPD用溅射靶。In order to solve the above-mentioned problems, the present inventors conducted extensive and intensive studies, and as a result, found that by configuring an ITO sputtering target with a plurality of divided targets and designing the edge portions of the plurality of divided targets, it is possible to provide a sputtering target that can be divided by arranging. On the other hand, by producing a large target, it is possible to reduce defective sputtering targets, especially sputtering targets for FPDs, which are caused by generation of particles at the edges of each divided target.

基于该发现,本发明提供:Based on this finding, the present invention provides:

1)一种ITO溅射靶,通过在背衬板上排列多个ITO分割靶并与该背衬板接合而构成,其中,仅在排列的ITO分割靶间的空隙侧的侧面具有选自铟、铟合金或锡合金的一种物质的覆盖层。1) An ITO sputtering target, which is constituted by arranging a plurality of ITO segmented targets on a backing plate and bonding to the backing plate, wherein only the side surface on the side of the gap between the arranged ITO segmented targets has indium , indium alloy or a coating of a substance of tin alloy.

另外,本发明提供:In addition, the present invention provides:

2)上述1)所述的ITO溅射靶,其特征在于,铟合金或锡合金为选自In-Sn、In-Bi、In-Bi-Sn、In-Ga、In-Ga-Sn、In-Ga-Bi、Sn-Ga、Sn-Bi和Sn-Ga-Bi中的任意一种物质。2) The ITO sputtering target described in 1) above, characterized in that the indium alloy or tin alloy is selected from In-Sn, In-Bi, In-Bi-Sn, In-Ga, In-Ga-Sn, In Any one of Ga-Bi, Sn-Ga, Sn-Bi and Sn-Ga-Bi.

另外,本发明提供:In addition, the present invention provides:

3)上述1)或2)所述的ITO溅射靶,其特征在于,ITO分割靶间的空隙为0.2~0.8mm。3) The ITO sputtering target described in 1) or 2) above, characterized in that the gap between the divided ITO targets is 0.2-0.8 mm.

另外,本发明提供:In addition, the present invention provides:

4)上述1)至3)中任一项所述的ITO溅射靶,其特征在于,覆盖层的厚度为0.04~0.35mm,并且从空隙的大小减去覆盖层的厚度得到的间隙的大小为0.1~0.72mm。4) The ITO sputtering target according to any one of the above 1) to 3), characterized in that the thickness of the cover layer is 0.04~0.35mm, and the size of the gap obtained by subtracting the thickness of the cover layer from the size of the gap 0.1~0.72mm.

发明效果Invention effect

这样制备的本发明的溅射靶,具有如下优点:可以提供即使在分割ITO靶的连续溅射时,也可以抑制结瘤的产生和异常放电,并且可以得到在与空隙部分相对的衬底上形成的膜的特性与其它部分的膜的特性无差异,即膜特性的均匀性高的膜的ITO溅射靶,特别是FPD用溅射靶,并且可以提高成膜的成品率,可以提高制品的品质。The sputtering target of the present invention prepared in this way has the following advantages: Even when continuous sputtering of the divided ITO target can be provided, the generation of nodules and abnormal discharge can be suppressed, and it can be obtained on the substrate opposite to the void portion. The characteristics of the formed film are no different from those of other parts of the film, that is, the ITO sputtering target of the film with high uniformity of film characteristics, especially the sputtering target for FPD, and can improve the yield of film formation and improve the quality of products. quality.

附图说明Description of drawings

图1是本发明的代表性ITO溅射靶的剖视说明图。FIG. 1 is an explanatory cross-sectional view of a typical ITO sputtering target of the present invention.

图2是以一定的间隔(空隙)排列的现有靶的说明图。FIG. 2 is an explanatory diagram of conventional targets arranged at constant intervals (gap).

具体实施方式Detailed ways

本发明的ITO溅射靶,是通过在背衬板上排列多个ITO分割靶并与该背衬板接合而构成的ITO溅射靶,其以仅在排列的ITO分割靶间的空隙侧的侧面具有选自铟、铟合金或锡合金的一种物质的覆盖层的结构的ITO溅射靶为基本。The ITO sputtering target of the present invention is an ITO sputtering target formed by arranging a plurality of ITO segmented targets on a backing plate and bonding to the backing plate, and it is formed only on the gap side between the arranged ITO segmented targets. An ITO sputtering target having a structure whose side is covered with a substance selected from indium, an indium alloy, or a tin alloy is basically used.

即,在背衬板上排列的多个ITO分割靶,各自的侧面没有紧贴,而是具有一定的间隔(空隙)。该示意图如图2所示。另一方面,说明本发明的代表性ITO溅射靶的剖视图如图1所示。That is, the side surfaces of the plurality of divided ITO targets arranged on the backing plate are not in close contact with each other, but have a certain interval (gap). The schematic diagram is shown in FIG. 2 . On the other hand, a cross-sectional view illustrating a representative ITO sputtering target of the present invention is shown in FIG. 1 .

该分割ITO靶的各构件,可以通过以下的方法制造。首先,称量氧化铟粉末和氧化锡粉末使得氧化锡为10重量%。Each member of this divided ITO target can be manufactured by the following method. First, indium oxide powder and tin oxide powder were weighed so that the tin oxide was 10% by weight.

通常的ITO的氧化锡浓度为10重量%,但是在作为透明导电体特性可以容许的范围内,可以将氧化锡的浓度设定在3~40重量%的范围。The usual ITO has a tin oxide concentration of 10% by weight, but the tin oxide concentration can be set in the range of 3 to 40% by weight within the allowable range for the properties of a transparent conductor.

然后,将称量的原料粉末进行利用湿式介质搅拌磨机等的混合粉碎,并进行用于提高流动性的造粒,在造粒时的浆料中,可以添加用于增加成形体强度的PVA等粘合剂。Then, the weighed raw material powder is mixed and pulverized by a wet media agitation mill, etc., and granulated for improving fluidity. In the slurry during granulation, PVA for increasing the strength of the molded body can be added. and other adhesives.

然后,进行压力成形后,在氧气气氛或大气气氛中进行常压烧结,得到ITO烧结体。Then, after pressure forming, normal-pressure sintering is performed in an oxygen atmosphere or an air atmosphere to obtain an ITO sintered body.

对所得到的ITO烧结体进行机械加工,得到分割ITO靶的各构件。此时,更优选对角进行倒角加工,进行减小表面粗糙度的加工。分割ITO靶的个数,例如为了适合FPD,可以根据大型ITO靶的尺寸确定。The obtained ITO sintered body was machined to obtain each member of the divided ITO target. In this case, it is more preferable to chamfer the corners to reduce the surface roughness. The number of divided ITO targets can be determined according to the size of a large ITO target, for example, in order to suit FPD.

这样的ITO靶,俯视一般为矩形,因此与此相对应,可以将多个长方形的分割ITO靶排列来制作。但是,分割ITO靶不限于长方形,当然也可以为其它形状例如正方形、三角形、扇形或者将它们适当组合来制作。本申请发明包括这些方面。Such an ITO target generally has a rectangular shape in plan view, and accordingly, a plurality of rectangular segmented ITO targets can be produced by arranging them. However, the segmented ITO target is not limited to a rectangle, and of course may be produced in other shapes such as a square, a triangle, a sector, or an appropriate combination thereof. The invention of the present application includes these aspects.

在通过上述方式制作的ITO靶的各构件的侧面覆盖铟或铟合金等,形成所述物质的覆盖层。形成该覆盖层的手段没有特别限制,例如可以使用下述用于在的背衬板上进行焊接的包含铟或铟合金的焊料来形成。作为其它手段,可以使用热喷涂法、镀敷法等。另外,可以仅将侧面通过电解进行还原而形成In系金属。Indium, an indium alloy, or the like is coated on the side surfaces of each member of the ITO target produced as described above to form a coating layer of the substance. The method for forming the covering layer is not particularly limited, and it can be formed using, for example, a solder containing indium or an indium alloy for soldering on a backing board described below. As other means, a thermal spraying method, a plating method, or the like can be used. In addition, only the side surface can be electrolytically reduced to form an In-based metal.

形成覆盖层后,使用包含铟或铟合金的焊料,如前述图1所示,在包含铜或铜合金的背衬板上进行焊接。After the covering layer is formed, soldering is performed on the backing board containing copper or copper alloy as shown in FIG. 1 above using solder containing indium or indium alloy.

之所以仅在侧面附加铟或铟合金等,是因为若不附加铟等,则容易产生以ITO靶的分割靶各构件间的空隙的端部为基点的异常放电等,另外,相反,若如现有例一样,在整个空隙中埋入铟等,则由该部分的上部形成的膜的电特性与由其它部分形成的膜的电特性不同。The reason why indium or indium alloy is only added to the side is that if no indium is added, abnormal discharges are likely to occur based on the end of the gap between the members of the divided target of the ITO target. In addition, on the contrary, if As in the conventional example, if indium or the like is buried in the entire space, the electrical characteristics of the film formed on the upper part of this part are different from those of the film formed on other parts.

ITO靶的分割靶各构件间的空隙(间隔)的调节是必要的,该空隙设定为0.2~0.8mm。此时的ITO分割靶间的空隙为形成覆盖层前的空隙。仅在ITO分割靶的空隙侧的侧面形成选自铟、铟合金或锡合金中的一种物质的覆盖层。然后,排列在背衬板上,并与背衬板接合。It is necessary to adjust the gap (interval) between each member of the divided target of the ITO target, and the gap is set to 0.2~0.8mm. The gap between the ITO divided targets at this time is the gap before the coating layer is formed. A coating layer of one substance selected from indium, an indium alloy, or a tin alloy is formed only on the side surface of the ITO split target on the side of the void. Then, it is aligned on the backing board and bonded to the backing board.

对于接合到背衬板上的各ITO分割靶而言,如上所述,需要一定的空隙,这是因为:该空隙小于0.2mm时,将多分割ITO靶的各构件粘贴到背衬板上后,难以防止接合层(使用焊料的焊接层)冷却时的热收缩造成的相邻靶构件间的碰撞引起的破损。For each ITO divided target bonded to the backing plate, as mentioned above, a certain gap is required. This is because: when the gap is less than 0.2 mm, after the members of the multi-segmented ITO target are pasted on the backing plate , it is difficult to prevent damage caused by collision between adjacent target members due to thermal contraction when the bonding layer (soldering layer using solder) is cooled.

另外,相反,大于0.8mm时,即使在各靶构件的侧面形成铟等,由侧面形成的膜的电特性也与靶构件稍有差异,因此由于空隙(间隔)过大会造成溅射时的膜的面内均匀性变差。In addition, on the contrary, when it is larger than 0.8mm, even if indium or the like is formed on the side surface of each target member, the electrical characteristics of the film formed on the side surface are slightly different from the target member, so the gap (interval) is too large to cause film damage during sputtering. The in-plane uniformity becomes worse.

另外,在ITO靶的溅射时及冷却时,或多或少会反复进行热膨胀和收缩,分割靶的空隙具有适度调节该热膨胀和收缩的功能,因此也具有可以防止靶的龟裂和破裂的效果。In addition, during the sputtering and cooling of the ITO target, thermal expansion and contraction are more or less repeated, and the gap between the divided targets has the function of moderately adjusting the thermal expansion and contraction, so it also has the function of preventing cracking and cracking of the target. Effect.

在各ITO分割靶的侧面形成的覆盖层的厚度设定为0.04~0.35mm。该覆盖层为相互面向空隙的单面的厚度。该覆盖层的目的在于,抑制结瘤的产生和异常放电,并且使得在与空隙部分相对的衬底上形成的膜的特性与其它部分的膜的特性无差异。The thickness of the coating layer formed on the side surface of each divided ITO target was set to 0.04 to 0.35 mm. The covering layer has the thickness of one side facing the voids. The purpose of this covering layer is to suppress the generation of nodules and abnormal discharge, and to make the characteristics of the film formed on the substrate opposite to the void portion not different from those of other portions.

覆盖层的厚度小于0.04mm时,没有该效果,超过0.35mm时,必须增大分割靶的空隙本身,膜的均匀性产生问题,因此优选将覆盖层的厚度设定为0.04~0.35mm。当然,要根据分割靶的空隙,在上述范围内调节覆盖层的厚度。以上的结果是,将从空隙的大小中减去覆盖层的厚度而得到的间隙的(大小)设定为0.1~0.72mm是合适的。When the thickness of the covering layer is less than 0.04 mm, this effect is lost, and when it exceeds 0.35 mm, the gap itself for dividing the target must be enlarged, causing problems with the uniformity of the film. Therefore, it is preferable to set the thickness of the covering layer to 0.04 to 0.35 mm. Of course, the thickness of the covering layer should be adjusted within the above range according to the gap of the divided target. From the above results, it is appropriate to set the gap (size) obtained by subtracting the thickness of the coating layer from the size of the gap to 0.1 to 0.72 mm.

作为在分割靶的侧面附加的材料,优选铟、铟合金、锡合金。这些金属或合金的熔点比较低,因此容易附加到侧面。另外,铟合金和锡合金的优选例子,可以列举:In-Sn、In-Bi、In-Bi-Sn、In-Ga、In-Ga-Sn、In-Ga-Bi、Sn-Ga、Sn-Bi和Sn-Ga-Bi。这些合金,特别是在与铟形成合金时,熔点比较低,为更优选的材料。As the material added to the side surface of the split target, indium, an indium alloy, and a tin alloy are preferable. These metals or alloys have relatively low melting points and are therefore easy to attach to the sides. In addition, preferred examples of indium alloys and tin alloys include: In-Sn, In-Bi, In-Bi-Sn, In-Ga, In-Ga-Sn, In-Ga-Bi, Sn-Ga, Sn- Bi and Sn-Ga-Bi. These alloys, especially when alloyed with indium, have a relatively low melting point and are more preferable materials.

实施例Example

以下,根据实施例和比较例进行说明。另外,本实施例仅仅是一例,本发明无论如何不限于该例。即,本发明仅由权利要求的范围限制,还包括本发明中所包含的实施例以外的各种变形。Hereinafter, it demonstrates based on an Example and a comparative example. In addition, this Example is just an example, and this invention is not limited to this example by any means. That is, the present invention is limited only by the scope of claims, and includes various modifications other than the examples included in the present invention.

(实施例1)(Example 1)

将作为原料的、比表面积5m2/g的氧化铟粉末和氧化锡粉末以重量比9:1的比例混合而成的混合粉末用基于球磨机的湿式介质搅拌磨机混合粉碎后,注入压模,以700kg/cm2的压力成形,制作ITO成形体。The mixed powder obtained by mixing indium oxide powder and tin oxide powder with a specific surface area of 5 m 2 /g as a raw material at a weight ratio of 9:1 is mixed and pulverized by a wet media agitation mill based on a ball mill, and then injected into a die. Forming with a pressure of 700kg/cm 2 produces an ITO molded body.

然后,将该ITO成形体在氧气气氛中以5℃/分钟的升温速度从室温升温到1500℃后,在1500℃保温20小时,然后,进行炉冷而烧结。Then, the ITO molded body was heated from room temperature to 1500° C. at a rate of 5° C./min in an oxygen atmosphere, then kept at 1500° C. for 20 hours, and then furnace-cooled and sintered.

将这样得到的烧结体的表面在平面磨床中使用400号金刚石磨粒磨削至厚度6.5mm,再将侧边用金刚石切刀切割为127mm×508mm尺寸,得到ITO靶构件。制作两块这样的加工体。The surface of the sintered body thus obtained was ground to a thickness of 6.5 mm using No. 400 diamond abrasive grains on a surface grinder, and the side was cut into a size of 127 mm×508 mm with a diamond cutter to obtain an ITO target member. Make two such processed bodies.

将这些烧结体设置到设定为200℃的热板上,升温后仅在侧面附加0.05mm厚的铟。These sintered bodies were placed on a hot plate set at 200° C., and after the temperature was raised, indium was attached to only the sides with a thickness of 0.05 mm.

然后,将无氧铜制的背衬板设置到设定为200℃的热板上,使用铟作为焊料,以其厚度为约0.2mm的方式进行涂布。在该背衬板上以0.4mm的空隙将通过上述方式在侧面附加有铟的两块ITO烧结体以接合面相互相对的方式设置,并自然冷却到室温。从上述可知,相邻的分割靶的覆盖层间的距离(间隔)为0.3mm。Then, a backing plate made of oxygen-free copper was placed on a hot plate set at 200° C., and indium was used as solder to coat the solder so that the thickness thereof was about 0.2 mm. The two ITO sintered bodies to which indium was added on the sides as described above were placed on the backing plate with a gap of 0.4 mm so that the bonding surfaces faced each other, and were naturally cooled to room temperature. From the above, it can be seen that the distance (interval) between the covering layers of adjacent divided targets is 0.3 mm.

将该靶安装到シンクロン制造的磁控溅射装置(BSC-7011)中,输入功率为,以DC电源2.3W/cm2,气压为0.6Pa,溅射气体为氩(Ar)并且气体流量为300sccm,进行到溅射累积电量为120WHr/cm2The target was installed in a magnetron sputtering device (BSC-7011) manufactured by Synkron, with an input power of 2.3 W/cm 2 from a DC power supply, a gas pressure of 0.6 Pa, argon (Ar) as a sputtering gas and a gas flow rate of 300 sccm, and the sputtering cumulative electric quantity is 120 WHr/cm 2 .

溅射中测定微弧产生的次数(次)。微弧的判断基准是,检测电压100V以上,释出能量(产生弧放电时的溅射电压×溅射电流×产生时间)为10mJ以下。The number (times) of micro-arc generation is measured during sputtering. The criterion for judging the micro-arc is that the detection voltage is 100V or more, and the released energy (sputtering voltage at the time of arc discharge x sputtering current x generation time) is 10mJ or less.

溅射累积电量为160WHr/cm2后,设置コ一ニング1737作为衬底,将膜厚设定为200nm,测定与空隙部相对的衬底面以及沿相反方向与其分别距离2cm和4cm的共计5个点的方块电阻,求出平均值和方块电阻的偏差(=100×2(最大方块电阻值-最小方块电阻值)/(最大方块电阻值+最小方块电阻值)%),以此评价膜电阻均匀性(R1)。After the sputtering cumulative electric quantity is 160WHr/cm 2 , set Corning 1737 as the substrate, set the film thickness to 200nm, and measure the substrate surface opposite to the void portion and a total of 5 samples at a distance of 2cm and 4cm from it in the opposite direction. The sheet resistance of the point, calculate the average value and the deviation of the sheet resistance (=100×2 (maximum sheet resistance value-minimum sheet resistance value)/(maximum sheet resistance value+minimum sheet resistance value)%) to evaluate the membrane resistance Uniformity (R1).

该实施例1的R1(5点的方块电阻、平均值、方块电阻的偏差)的结果如表1所示。Table 1 shows the results of R1 (sheet resistance at 5 points, average value, and variation of sheet resistance) in Example 1.

另外,空隙、铟等在空隙上的附着状态、直到累积120WHr/cm2为止的微弧放电产生累积次数、膜特性等结果也一并示于表1中。In addition, results such as voids, the state of adhesion of indium, etc. to the voids, the cumulative number of micro-arc discharge occurrences up to a cumulative 120 WHr/cm 2 , and film properties are also shown in Table 1.

表1Table 1

如上述表1、图1所示,在实施例1的分割靶的侧面覆盖的材料为铟(In),覆盖层的厚度为0.05mm,空隙为0.4mm,微弧的产生次数为260次,方块电阻的平均值为10.3Ω/□,方块电阻的偏差为7.3%,得到方块电阻的平均值为适度的数值,方块电阻的偏差小,微弧的产生次数少的结果。As shown in the above Table 1 and Figure 1, the material covered on the side surface of the divided target in Example 1 is indium (In), the thickness of the covering layer is 0.05 mm, the gap is 0.4 mm, and the number of micro-arcs is 260 times. The average value of the sheet resistance was 10.3Ω/□, and the variation of the sheet resistance was 7.3%. The average value of the sheet resistance was a moderate value, the variation of the sheet resistance was small, and the number of occurrences of micro-arcs was small.

ITO的情况下,可以通过方块电阻评价衬底上膜的特性,象这样方块电阻的变动少,意味着在衬底上均匀地成膜。In the case of ITO, the properties of the film on the substrate can be evaluated by the sheet resistance, and the small variation in the sheet resistance means that the film is formed uniformly on the substrate.

(实施例2)(Example 2)

除了将覆盖层的厚度变为0.1mm以外,在与实施例1同样的条件下进行。该结果同样地如表1、图1所示。相邻的分割靶的覆盖层间的距离(间隔)为0.2mm。It carried out under the same conditions as Example 1 except having changed the thickness of a cover layer into 0.1 mm. The results are similarly shown in Table 1 and FIG. 1 . The distance (interval) between the covering layers of adjacent divided targets was 0.2 mm.

微弧的产生次数为232次,方块电阻的平均值为10.2Ω/□,方块电阻的偏差为7.0%,得到方块电阻为适度的数值,方块电阻的偏差小,微弧的产生次数少的结果。The number of occurrences of micro-arcs was 232 times, the average value of the square resistance was 10.2Ω/□, and the deviation of the square resistance was 7.0%. The result was that the square resistance was a moderate value, the deviation of the square resistance was small, and the number of occurrences of micro-arcs was small. .

ITO的情况下,可以通过方块电阻评价衬底上膜的特性,象这样方块电阻的变动少,意味着在衬底上均匀地成膜。In the case of ITO, the properties of the film on the substrate can be evaluated by the sheet resistance, and the small variation in the sheet resistance means that the film is formed uniformly on the substrate.

(实施例3)(Example 3)

除了将空隙变为0.2mm以外,在与实施例1同样的条件下进行。相邻的分割靶的覆盖层间的距离(间隔)为0.1mm。该结果同样如表1、图1所示。It carried out under the same conditions as Example 1 except having changed the gap into 0.2 mm. The distance (interval) between the covering layers of adjacent divided targets was 0.1 mm. The results are also shown in Table 1 and FIG. 1 .

微弧的产生次数为210次,方块电阻的平均值为10.3Ω/□,方块电阻的偏差为4.9%,得到方块电阻为适度的数值,方块电阻的偏差小,微弧的产生次数少的结果。The number of occurrences of micro-arcs was 210 times, the average value of sheet resistance was 10.3Ω/□, and the variation of sheet resistance was 4.9%. The result was that the sheet resistance was moderate, the variation of sheet resistance was small, and the number of occurrences of micro-arcs was small. .

ITO的情况下,可以通过方块电阻评价衬底上膜的特性,象这样方块电阻的变动少,意味着在衬底上均匀地成膜。In the case of ITO, the properties of the film on the substrate can be evaluated by the sheet resistance, and the small variation in the sheet resistance means that the film is formed uniformly on the substrate.

(实施例4)(Example 4)

除了将附加到ITO分割靶侧面的铟变为锡浓度为10原子%的In-Sn合金以外,在与实施例1同样的条件下进行。该结果同样如表1、图1所示。相邻的分割靶的覆盖层间的距离(间隔)为0.3mm。It carried out under the same conditions as Example 1 except having changed the indium attached to the side surface of the ITO split target into the In-Sn alloy whose tin concentration was 10 at%. The results are also shown in Table 1 and FIG. 1 . The distance (interval) between the covering layers of adjacent divided targets was 0.3 mm.

微弧的产生次数为212次,方块电阻的平均值为10.4Ω/□,方块电阻的偏差为5.8%,得到方块电阻为适度的数值,方块电阻的偏差小,微弧的产生次数少的结果。The number of occurrences of micro-arcs was 212 times, the average value of the square resistance was 10.4Ω/□, and the deviation of the square resistance was 5.8%. The result was that the square resistance was a moderate value, the deviation of the square resistance was small, and the number of occurrences of micro-arcs was small. .

ITO的情况下,可以通过方块电阻评价衬底上膜的特性,象这样方块电阻的变动少,意味着在衬底上均匀地成膜。In the case of ITO, the properties of the film on the substrate can be evaluated by the sheet resistance, and the small variation in the sheet resistance means that the film is formed uniformly on the substrate.

(比较例1)(comparative example 1)

除了在ITO分割靶侧面什么也不附加,将分割靶的空隙设定为0.4mm以外,在与实施例1同样的条件下进行。该结果同样如表1所示。另外,由于在ITO分割靶侧面未形成覆盖层,因此结构方面如图2所示。It carried out under the same conditions as Example 1 except not adding anything to the side surface of an ITO split target, but having set the space|gap of a split target to 0.4 mm. The results are also shown in Table 1. In addition, since no cover layer is formed on the side surface of the ITO split target, the structure is as shown in FIG. 2 .

微弧的产生次数为750次,方块电阻的平均值为10.2Ω/□,方块电阻的偏差为3.9%,得到方块电阻的平均值为适度的数值,方块电阻的偏差小,但是微弧的产生次数极多的结果。The number of occurrences of micro-arc is 750 times, the average value of square resistance is 10.2Ω/□, and the deviation of square resistance is 3.9%. Too many results.

(比较例2)(comparative example 2)

除了在ITO分割靶侧面附加0.02mm的In以外,在与实施例1同样的条件下进行。该结果同样如表1、图1所示。另外,相邻分割靶的覆盖层间的距离(间隔)为0.3mm。It carried out under the same conditions as Example 1 except having added 0.02 mm of In to the side surface of the ITO split target. The results are also shown in Table 1 and FIG. 1 . In addition, the distance (interval) between the covering layers of adjacent divided targets was 0.3 mm.

微弧的产生次数为736次,方块电阻的平均值为10.2Ω/□,方块电阻的偏差为3.9%,得到方块电阻的平均值为适度的数值,方块电阻的偏差小,但是微弧的产生次数极多的结果。The number of occurrences of micro-arc was 736 times, the average value of the square resistance was 10.2Ω/□, and the deviation of the square resistance was 3.9%. Too many results.

(比较例3)(comparative example 3)

除了在ITO分割靶侧面什么也不附加,将分割靶的空隙设定为0.2mm以外,在与实施例1同样的条件下进行。该结果同样如表1所示。另外,由于在ITO分割靶侧面未形成覆盖层,因此结构方面如图2所示。It carried out under the same conditions as Example 1 except not adding anything to the side surface of the ITO split target, and setting the gap of the split target at 0.2 mm. The results are also shown in Table 1. In addition, since no cover layer is formed on the side surface of the ITO split target, the structure is as shown in FIG. 2 .

微弧的产生次数为508次,方块电阻为10.2Ω/□,方块电阻的偏差为3.0%,得到方块电阻的平均值为适度的数值,方块电阻的偏差小,微弧的产生次数虽然与比较例1相比稍有减少,但是仍然极多的结果。The number of occurrences of micro-arc is 508 times, the square resistance is 10.2Ω/□, and the deviation of square resistance is 3.0%. The average value of square resistance obtained is a moderate value, and the deviation of square resistance is small. Slightly reduced compared to Example 1, but still extremely large results.

(比较例4)(comparative example 4)

将分割靶的配置即分割靶间的空隙设定为0.4mm,但是在ITO分割靶间埋入铟(In)。分割靶间有空隙,但是其间放入其它物质,从而成为间隙实质上消失的状态。除此以外,在与实施例1同样的条件下进行。该结果同样如表1所示。The arrangement of the split targets, that is, the gap between the split targets was set to 0.4 mm, but indium (In) was embedded between the ITO split targets. There are gaps between the divided targets, but other substances are put in between, and the gaps are substantially eliminated. Except for this, it carried out under the same conditions as Example 1. The results are also shown in Table 1.

微弧的产生次数为240次,方块电阻的平均值为9.4Ω/□,方块电阻的偏差为38.2%,微弧的产生次数与实施例相同程度,但是方块电阻的平均值差,方块电阻的偏差极大。The generation number of micro-arc is 240 times, the average value of square resistance is 9.4Ω/□, the deviation of square resistance is 38.2%, the generation number of micro-arc is the same degree as embodiment, but the average value of square resistance is poor, the square resistance The deviation is huge.

ITO的情况下,可以通过方块电阻评价衬底上膜的特性,象这样方块电阻的变动大,意味着在衬底上没有均匀地成膜。In the case of ITO, the properties of the film on the substrate can be evaluated by the sheet resistance, and a large variation in the sheet resistance means that the film is not formed uniformly on the substrate.

(比较例5)(comparative example 5)

将分割靶的配置即分割靶间的空隙设定为0.2mm,但是在ITO分割靶间埋入铟(In)。分割靶间有空隙,但是其间放入其它物质,从而成为间隙实质上消失的状态。除此以外,在与实施例1同样的条件下进行。结果同样如表1所示。The arrangement of the split targets, that is, the gap between the split targets was set to 0.2 mm, but indium (In) was embedded between the ITO split targets. There are gaps between the divided targets, but other substances are put in between, and the gaps are substantially eliminated. Except for this, it carried out under the same conditions as Example 1. The results are also shown in Table 1.

微弧的产生次数为198次,方块电阻的平均值为9.9Ω/□,方块电阻的偏差为17.6%,微弧的产生次数与实施例大致相同程度,但是方块电阻的平均值差,方块电阻的偏差极大。The number of times of generation of micro-arc is 198 times, the average value of square resistance is 9.9Ω/□, the deviation of square resistance is 17.6%, the number of times of generation of micro-arc is about the same degree as the embodiment, but the average value of square resistance is poor, square resistance The deviation is extremely large.

ITO的情况下,可以通过方块电阻评价衬底上膜的特性,象这样方块电阻的变动大,意味着在衬底上没有均匀地成膜。In the case of ITO, the properties of the film on the substrate can be evaluated by the sheet resistance, and a large variation in the sheet resistance means that the film is not formed uniformly on the substrate.

从上述的实施例、比较例明显可以看出,在背衬板上排列多个ITO分割靶并与该背衬板接合而构成的ITO溅射靶,具有仅在排列的ITO分割靶间的空隙侧的侧面具有选自铟、铟合金或锡合金的一种物质的覆盖层的结构是极其重要的。It is clear from the above-mentioned examples and comparative examples that the ITO sputtering target formed by arranging a plurality of ITO segmented targets on a backing plate and bonding to the backing plate has a space only between the arranged ITO segmented targets. It is extremely important that the sides of the sides have a covering layer of a substance selected from indium, an indium alloy or a tin alloy.

由此,可以抑制结瘤的产生和异常放电,并且可以得到在与空隙部分相对的衬底上形成的膜的特性与其它部分的膜特性无差异,即膜特性的均匀性高的膜。Accordingly, nodulation and abnormal discharge can be suppressed, and a film formed on the substrate opposite to the void can have the same film properties as other parts, that is, a film with high uniformity in film properties can be obtained.

产业实用性Industrial applicability

本发明的溅射靶,具有如下显著优点:可以提供即使在分割ITO靶的连续溅射时,也可以抑制结瘤的产生和异常放电,并且可以得到在与空隙部分相对的衬底上形成的膜的特性与其它部分的膜的特性无差异,即膜特性的均匀性高的膜的ITO溅射靶,并且可以提高成膜的成品率,可以提高制品的品质,从而可以提供能够减少由分割靶部引起的粉粒产生造成的不合格率的大型溅射靶,因此特别是作为FPD用溅射靶是有用的。The sputtering target of the present invention has the following remarkable advantages: Even when continuous sputtering of the divided ITO target can be provided, the generation of nodules and abnormal discharge can be suppressed, and the sputtering target formed on the substrate opposite to the void portion can be obtained. The characteristics of the film are no different from those of other parts of the film, that is, the ITO sputtering target of the film with high uniformity of film characteristics, and can improve the yield of film formation, improve the quality of the product, and thus provide the ability to reduce the cost caused by segmentation. Since it is a large sputtering target with a high failure rate due to particle generation at the target portion, it is especially useful as a sputtering target for FPDs.

Claims (3)

1.一种ITO溅射靶,通过在背衬板上排列多个ITO分割靶并与该背衬板接合而构成,其中,仅在排列的ITO分割靶间的空隙侧的侧面具有选自铟、铟合金或锡合金的一种物质的覆盖层,1. An ITO sputtering target, constituted by arranging a plurality of ITO segmented targets on a backing plate and bonding to the backing plate, wherein only the side surfaces on the side of the gap between the arranged ITO segmented targets have indium , an indium alloy or a coating of a substance of a tin alloy, 覆盖层的厚度为0.04~0.35mm,并且从空隙的大小减去覆盖层的厚度得到的间隙的大小为0.1~0.72mm。The thickness of the cover layer is 0.04 to 0.35 mm, and the size of the gap obtained by subtracting the thickness of the cover layer from the size of the void is 0.1 to 0.72 mm. 2.如权利要求1所述的ITO溅射靶,其特征在于,铟合金或锡合金为选自In-Sn、In-Bi、In-Bi-Sn、In-Ga、In-Ga-Sn、In-Ga-Bi、Sn-Ga、Sn-Bi和Sn-Ga-Bi中的任意一种物质。2. ITO sputtering target as claimed in claim 1, is characterized in that, indium alloy or tin alloy is selected from In-Sn, In-Bi, In-Bi-Sn, In-Ga, In-Ga-Sn, Any one of In-Ga-Bi, Sn-Ga, Sn-Bi and Sn-Ga-Bi. 3.如权利要求1或2所述的ITO溅射靶,其特征在于,ITO分割靶间的空隙为0.2~0.8mm。3. The ITO sputtering target according to claim 1 or 2, wherein the gap between the divided ITO targets is 0.2-0.8 mm.
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