TW201900581A - Sn-Zn-O based oxide sintered body and method for producing same - Google Patents

Sn-Zn-O based oxide sintered body and method for producing same Download PDF

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TW201900581A
TW201900581A TW107106493A TW107106493A TW201900581A TW 201900581 A TW201900581 A TW 201900581A TW 107106493 A TW107106493 A TW 107106493A TW 107106493 A TW107106493 A TW 107106493A TW 201900581 A TW201900581 A TW 201900581A
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桒原正和
仁藤茂生
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日商住友金屬鑛山股份有限公司
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Abstract

Provided are an Sn-Zn-O-based oxide sintered body of high density and low resistance that can be used in such applications as barrier films and protective films, and a production method therefor. This Sn-Zn-O-based oxide sintered body has zinc (Zn) and tin (Sn) as components, and additionally contains at least germanium (Ge), tantalum (Ta), and gallium (Ga) as components, the metal atom number ratios being between 0.1 and 0.3 inclusive for Sn/(Zn+Sn), between 0.0005 and 0.01 inclusive for Ge/(Zn + Sn + Ge + Ta + Ga), between 0.0005 and 0.01 inclusive for Ta/(Zn + Sn + Ge + Ta + Ga), and between 0.001 and 0.1 inclusive for Ga/(Zn + Sn + Ge + Ta + Ga), the specific resistance thereof being between 5 [Omega].cm and 12,000 [Omega].m inclusive, and the relative density thereof being 94% or greater.

Description

Sn-Zn-O系氧化物燒結體及其製造方法Sn-zn-O series oxide sintered body and manufacturing method thereof

本發明係關於在以直流濺鍍、高頻濺鍍之濺鍍法來製造適用於太陽能電池、液晶表面元件、觸控面板等之透明導電膜時,作為濺鍍靶材所使用之Sn-Zn-O系氧化物燒結體及其製造方法者。本申請案係以在日本於2017年5月12日所申請之日本專利申請號碼特願2017-095982作為基礎而主張優先權者,其申請內容係藉由參照而援用於本申請案中。The invention relates to Sn-Zn used as a sputtering target when manufacturing a transparent conductive film suitable for solar cells, liquid crystal surface elements, touch panels, and the like by a sputtering method of direct current sputtering and high frequency sputtering. -O-based oxide sintered body and its production method. This application claims priority based on Japanese Patent Application No. 2017-095982 filed in Japan on May 12, 2017, and its application content is incorporated herein by reference.

具有高導電性與可見光區域中之高透過率的透明導電膜除了被利用於太陽能電池、液晶顯示元件、有機電致發光及無機電致發光等之表面元件、或觸控面板用電極等以外,亦被利用作為汽車窗或建築用之熱射線反射膜、抗靜電膜、冷凍展示櫃、保護膜等之各種的防霧用透明發熱體。Transparent conductive films having high conductivity and high transmittance in the visible light region are used in surface elements such as solar cells, liquid crystal display elements, organic electroluminescence and inorganic electroluminescence, and electrodes for touch panels, etc. It is also used as various anti-fog transparent heating elements such as heat ray reflection film, antistatic film, refrigerated display cabinet, protective film, etc. for automobile windows or buildings.

作為透明導電膜,已知有包含銻或氟作為摻雜劑的氧化錫(SnO2 )、包含鋁或鎵作為摻雜劑的氧化鋅(ZnO)、及包含錫作為摻雜劑的氧化銦(In2 O3 )等。尤其,包含錫作為摻雜劑的氧化銦(In2 O3 )膜,亦即,In-Sn-O系之膜係被稱為ITO(Indium tin oxide)膜,由於是容易得到低電阻的膜,而被廣泛使用。As the transparent conductive film, tin oxide (SnO 2 ) containing antimony or fluorine as a dopant, zinc oxide (ZnO) containing aluminum or gallium as a dopant, and indium oxide (tin oxide) containing tin as a dopant are known. In 2 O 3 ). In particular, an indium oxide (In 2 O 3 ) film containing tin as a dopant, that is, an In-Sn-O-based film system is called an ITO (Indium tin oxide) film, because it is a film with low resistance that is easy to obtain. And is widely used.

作為上述透明導電膜之製造方法常使用有直流濺鍍、高頻濺鍍之濺鍍法。在以蒸氣壓低的材料之成膜或精密的膜厚控制為必要時,濺鍍法係為有效的手法,由於操作非常簡便,因此工業性廣泛地利用。As a method for manufacturing the transparent conductive film, a sputtering method using direct current sputtering and high frequency sputtering is often used. The sputtering method is an effective method when film formation of a material having a low vapor pressure or precise film thickness control is necessary. Since the operation is very simple, it is widely used industrially.

為了製造上述透明導電膜,以往,廣範圍地使用有ITO等之氧化銦系的材料。但,銦金屬在地球上為稀少金屬且具有毒性,因此,對於環境或人體有不良影響的疑慮,而需要有非銦系的材料。In order to manufacture the transparent conductive film, conventionally, an indium oxide-based material such as ITO has been widely used. However, indium metal is a rare metal on the earth and is toxic. Therefore, it is necessary to have a non-indium-based material because of doubts about adverse effects on the environment or human body.

作為上述非銦系的材料,如上述般地,已知有包含鋁或鎵作為摻雜劑的氧化鋅(ZnO)系材料、及包含銻或氟作為摻雜劑的氧化錫(SnO2 )系材料。並且,上述氧化鋅(ZnO)系材料之透明導電膜係以濺鍍法來工業性製造,但,具有耐藥品性(耐鹼性、耐酸性)缺乏等的缺點。另一方面,氧化錫(SnO2 )系材料之透明導電膜雖為耐藥品性優異者,但難以製造高密度且具耐久性之氧化錫系燒結體靶材,因此,具有伴隨難以利用濺鍍法來製造上述透明導電膜的缺點。As the non-indium-based material, as described above, a zinc oxide (ZnO) -based material containing aluminum or gallium as a dopant and a tin oxide (SnO 2 ) -based material containing antimony or fluorine as a dopant are known. material. In addition, the transparent conductive film of the zinc oxide (ZnO) -based material is industrially manufactured by a sputtering method, but has disadvantages such as lack of chemical resistance (alkali resistance, acid resistance) and the like. On the other hand, although a transparent conductive film of a tin oxide (SnO 2 ) -based material is excellent in chemical resistance, it is difficult to manufacture a high-density and durable tin oxide-based sintered body target. Therefore, it is accompanied by difficulty in using sputtering. Disadvantages of manufacturing the above-mentioned transparent conductive film.

因此,作為改善該等缺點的材料,提案有以氧化鋅與氧化錫作為主成分的燒結體。例如,於專利文獻1中記載有一種Zn-Sn-O系氧化物燒結體,其係不含有氧化錫之結晶相或固溶有鋅的氧化錫之結晶相,而是以氧化鋅相與錫酸鋅化合物相所構成,或以錫酸鋅化合物相所構成。Therefore, as a material for improving these disadvantages, a sintered body having zinc oxide and tin oxide as main components has been proposed. For example, Patent Document 1 describes a Zn-Sn-O-based oxide sintered body which does not contain a crystalline phase of tin oxide or a crystalline phase of tin oxide in which zinc is solid-dissolved, but uses a zinc oxide phase and tin A zinc acid compound phase or a zinc stannate compound phase.

又,於專利文獻2中記載有一種燒結體,其係平均結晶粒徑為4.5μm以下,且當將使用有CuKα射線之X射線繞射之Zn2 SnO4 相中的(222)面、(400)面之累積強度設為I(222) 、I(400) 時,以I(222) /[I(222) +I(400) ]所表示之配向度為比標準(0.44)更大的0.52以上。再者,於專利文獻2中亦記載有作為製造具備有上述特性之燒結體的方法而以下列步驟來構成該燒結體之製造步驟的方法,該步驟為:於燒成爐內,在包含氧的環境中,以800℃~1400℃之條件,將成形體進行燒成的步驟;與在最高燒成溫度下之保持結束後,使燒成爐內成為Ar氣體等之惰性環境來進行冷卻的步驟。 [先前技術文獻] [專利文獻]Further, Patent Document 2 describes a sintered body having an average crystal grain size of 4.5 μm or less and a (222) plane in a Zn 2 SnO 4 phase using X-ray diffraction using CuKα rays, ( When the cumulative intensity of the 400) plane is set to I (222) and I (400) , the orientation degree represented by I (222) / [I (222) + I (400) ] is greater than the standard (0.44) 0.52 or more. Furthermore, Patent Document 2 also describes a method for forming a sintered body as a method of producing a sintered body having the above-mentioned characteristics by the following steps. This step is to include oxygen in a firing furnace in a firing furnace. In the environment of 800 ° C to 1400 ° C, firing the compact; and after the holding at the highest firing temperature is completed, the firing furnace is cooled to an inert environment such as Ar gas for cooling. step. [Prior Art Literature] [Patent Literature]

[專利文獻1]日本特開2007-277075號公報   [專利文獻2]日本特開2013-036073號公報[Patent Document 1] Japanese Patent Laid-Open No. 2007-277075 [Patent Document 2] Japanese Patent Laid-Open No. 2013-036073

[發明所欲解決之課題][Problems to be Solved by the Invention]

然而,於該等方法中,於以Zn及Sn作為主成分之Sn-Zn-O系氧化物燒結體中,雖可得到能承受機械性強度之燒結體強度,但難以得到充分的密度或導電性,作為對在量產現場之濺鍍成膜所必要的特性並無法滿足。亦即,於常壓燒結法中,在達到燒結體之高密度化或導電性之點上仍留有課題。However, in these methods, although the strength of a sintered body capable of withstanding mechanical strength can be obtained in a Sn-Zn-O-based oxide sintered body containing Zn and Sn as main components, it is difficult to obtain sufficient density or conductivity. The performance is not sufficient as a characteristic necessary for sputtering film formation at a mass production site. That is, in the normal pressure sintering method, there is still a problem in terms of achieving high density or conductivity of the sintered body.

以Zn及Sn作為主成分之Sn-Zn-O系氧化物燒結體,係用難以具備高密度且低電阻之兩特性的材料,即使改變Sn與Zn之摻合比,也難以製作高密度且導電性優異的氧化物燒結體。於燒結體密度中,雖藉由摻合比而存在有些許的密度上下變動,但針對導電性,顯示1×106 Ω・cm以上之非常高的比電阻值,而導電性缺乏。The Sn-Zn-O based oxide sintered body containing Zn and Sn as main components is made of a material which is difficult to have both characteristics of high density and low resistance. Even if the blending ratio of Sn and Zn is changed, it is difficult to produce a high density An oxide sintered body having excellent conductivity. Although the density of the sintered body varies slightly depending on the blending ratio, it exhibits a very high specific resistance value of 1 × 10 6 Ω ・ cm or more for conductivity, and lacks conductivity.

於以Zn及Sn作為主成分之Sn-Zn-O系氧化物燒結體之製作中,從1100℃附近起開始生成Zn2 SnO4 之化合物,超過1400℃後Zn之揮發開始,1450℃附近起Zn之揮發變得明顯。若為了提昇Sn-Zn-O系氧化物燒結體的密度而以高溫進行燒成,則由於Zn之揮發進行,因此粒界擴散或粒彼此之結合為弱,而無法得到高密度之氧化物燒結體。In the production of Sn-Zn-O based oxide sintered bodies with Zn and Sn as the main components, Zn 2 SnO 4 compounds start to be generated near 1100 ° C, and the volatilization of Zn starts at around 1400 ° C, starting from around 1450 ° C. Volatilization of Zn becomes apparent. If the firing is performed at a high temperature in order to increase the density of the Sn-Zn-O-based oxide sintered body, the volatilization of Zn progresses, so the grain boundary diffusion or the combination of grains is weak, and high density oxide sintering cannot be obtained. body.

又,針對導電性,由於Zn2 SnO4 、ZnO、SnO2 為導電性缺乏的物質,因此即使調整摻合比來調整化合物相或ZnO、SnO2 的量,亦無法將導電性大幅地改善。Regarding conductivity, since Zn 2 SnO 4 , ZnO, and SnO 2 are substances lacking conductivity, even if the blending ratio is adjusted to adjust the amount of the compound phase or the amount of ZnO and SnO 2 , the conductivity cannot be significantly improved.

以往所使用之ITO的燒結體之比電阻值為2~3×10-4 Ω・cm,藉由以此燒結體作為靶材來進行濺鍍而適宜使用作為液晶或太陽能電池等之透明導電膜。另一方面,近年來,存在有導電性雖比ITO差,但可使用於氣體阻隔膜、水蒸氣阻隔膜等之阻隔膜或保護以避免損傷或衝擊之保護膜等的用途中,且比電阻值為10Ω・cm~×104 Ω・cm左右的要求。因而,要求有適於該等條件之Sn-Zn-O系氧化物燒結體。The sintered body of ITO used in the past has a specific resistance value of 2 to 3 × 10 -4 Ω ・ cm. The sintered body is used as a target for sputtering, and it is suitable to be used as a transparent conductive film such as a liquid crystal or a solar cell. . On the other hand, in recent years, although the conductivity is lower than that of ITO, there are applications in which it can be used as a barrier film such as a gas barrier film, a water vapor barrier film, or a protective film to protect it from damage or impact. The value is about 10Ω ・ cm ~ × 10 4 Ω ・ cm. Therefore, a Sn-Zn-O-based oxide sintered body suitable for these conditions is required.

因此,本發明之課題在於,提供可使用於阻隔膜或保護膜等之用途中,高密度且低電阻的Sn-Zn-O系氧化物燒結體及其製造方法。 [用以解決課題之手段]Therefore, an object of the present invention is to provide a Sn-Zn-O-based oxide sintered body with high density and low resistance, which can be used in applications such as barrier films and protective films, and a method for producing the same. [Means to solve the problem]

本發明者們,發現為了解決上述課題,藉由以作為原子數比Sn/(Sn+Zn)為0.1以上0.3以下之比例包含Sn,且作為添加元素而以特定的比例含有Ge、Ta、Ga 3種,而可得到適於阻隔膜或保護膜等之用途之比電阻值為10Ω・cm~×104 Ω・cm左右且高密度的Sn-Zn-O系氧化物燒結體,因而完成本發明。The present inventors have found that in order to solve the above-mentioned problems, Sn is contained in a ratio of Sn / (Sn + Zn) of 0.1 to 0.3 as an atomic ratio, and Ge, Ta, and Ga are contained in a specific ratio as an additive element. Three kinds of Sn-Zn-O-based oxide sintered bodies having a specific resistance value of about 10Ω ・ cm ~ × 10 4 Ω ・ cm suitable for applications such as a barrier film or a protective film can be obtained. invention.

亦即,本發明之一樣態係具有鋅(Zn)與錫(Sn)作為成分之Sn-Zn-O系氧化物燒結體,其中,進一步含有至少鍺(Ge)、鉭(Ta)、及鎵(Ga)作為成分,且金屬原子數比係Sn/(Zn+Sn)為0.1以上0.3以下、Ge/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、Ta/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、Ga/(Zn+Sn+Ge+Ta+Ga)為0.001以上0.1以下,比電阻為5Ω・cm以上12000Ω・cm以下,相對密度為94%以上。That is, the homogeneous system of the present invention is a Sn-Zn-O-based oxide sintered body having zinc (Zn) and tin (Sn) as components, and further containing at least germanium (Ge), tantalum (Ta), and gallium. (Ga) as a component, and the metal atomic ratio Sn / (Zn + Sn) is 0.1 or more and 0.3 or less, Ge / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less, and Ta / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less, Ga / (Zn + Sn + Ge + Ta + Ga) is 0.001 or more and 0.1 or less, the specific resistance is 5Ω ・ cm or more and 12000Ω ・ cm or less, and the relative density is 94% or more. .

依據本發明之一樣態,藉由以使Sn/(Sn+Zn)成為0.1以上0.3以下的比例,且作為添加元素而使用鍺(Ge)、鉭(Ta)、及鎵(Ga)3種,而可設為可使用於阻隔膜或保護膜等之用途中,高密度且低電阻的Sn-Zn-O系氧化物燒結體。According to the state of the present invention, three types of germanium (Ge), tantalum (Ta), and gallium (Ga) are used as an additive element such that Sn / (Sn + Zn) is at a ratio of 0.1 to 0.3, In addition, it can be a Sn-Zn-O-based oxide sintered body which can be used in applications such as a barrier film or a protective film with high density and low resistance.

此時,於本發明之一樣態中,可設為金屬原子數比係Sn/(Zn+Sn)為0.16以上0.23以下,比電阻為5Ω・cm以上110Ω・cm以下,相對密度為98%以上。At this time, in the state of the present invention, the metal atomic ratio system Sn / (Zn + Sn) can be set to be 0.16 or more and 0.23 or less, the specific resistance is 5Ω ・ cm or more and 110Ω ・ cm or less, and the relative density is 98% or more. .

如此般,藉由更加限定Sn/(Zn+Sn),而可進一步實現高密度且低電阻的Sn-Zn-O系氧化物燒結體。As such, by further limiting Sn / (Zn + Sn), a Sn-Zn-O-based oxide sintered body having a high density and a low resistance can be further realized.

又,於本發明之一樣態中,於Sn-Zn-O系氧化物燒結體中,可設為纖鋅礦型結晶構造之ZnO相為全體的5~70%(於本說明書中,「~」係設為意味著下限以上、上限以下者,以下相同)之範圍,或是尖晶石型結晶構造之Zn2 SnO4 相為全體的30~95%之範圍所構成。In the aspect of the present invention, in the Sn-Zn-O-based oxide sintered body, the wurtzite-type crystal structure of the ZnO phase may be 5 to 70% of the whole (in this specification, "~ ”Means a range that means the lower limit is greater than the upper limit, and the same applies below), or the Zn 2 SnO 4 phase with a spinel crystal structure is in a range of 30 to 95% of the total.

藉由設為如本發明之一樣態般的金屬原子數比,而成為藉由上述結晶構造所構成的Sn-Zn-O系氧化物燒結體。By setting the metal atomic ratio as in the present invention, a Sn-Zn-O-based oxide sintered body having the above-mentioned crystal structure is obtained.

又,本發明之另一樣態係具有鋅(Zn)與錫(Sn)作為成分之Sn-Zn-O系氧化物燒結體之製造方法,其中,具有下列步驟:將鋅之氧化物粉末、錫之氧化物粉末、及含有添加元素之氧化物粉末進行混合而製作造粒粉末的造粒工程;將前述造粒粉末進行加壓成形而得到成形體的成形步驟;以及將前述成形體進行燒成而得到氧化物燒結體的燒成步驟,前述添加元素至少為鍺(Ge)、鉭(Ta)、及鎵(Ga),以使金屬原子數比成為Sn/(Zn+Sn)為0.1以上0.3以下、Ge/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、Ta/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、Ga/(Zn+Sn+Ge+Ta+Ga)為0.001以上0.1以下的方式來將前述鋅之氧化物粉末、前述錫之氧化物粉末、及前述含有添加元素之氧化物粉末進行混合。Also, another aspect of the present invention is a method for producing a sintered body of Sn-Zn-O oxide having zinc (Zn) and tin (Sn) as components, which includes the following steps: powder of zinc oxide, tin A granulation process for preparing a granulated powder by mixing an oxide powder and an oxide powder containing an additive element; a forming step of pressing the granulated powder to obtain a formed body; and firing the formed body In the firing step of obtaining an oxide sintered body, the aforementioned additional elements are at least germanium (Ge), tantalum (Ta), and gallium (Ga) so that the metal atomic ratio becomes Sn / (Zn + Sn) of 0.1 or more and 0.3 or less. Below, Ge / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less, Ta / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less, Ga / (Zn + Sn + Ge + Ta + Ga) is 0.001 or more and 0.1 or less to mix the zinc oxide powder, the tin oxide powder, and the additive element-containing oxide powder.

依據本發明之另一樣態,藉由以使Sn/(Zn+Sn)成為0.1以上0.3以下的比例,且作為添加元素而將鍺(Ge)、鉭(Ta)、及鎵(Ga)3種以特定的比例進行混合,而可製造可使用於阻隔膜或保護膜等之用途中,高密度且低電阻的Sn-Zn-O系氧化物燒結體。According to another aspect of the present invention, three types of germanium (Ge), tantalum (Ta), and gallium (Ga) are used as an additive element so that Sn / (Zn + Sn) becomes a ratio of 0.1 to 0.3. By mixing in a specific ratio, a high density and low resistance Sn-Zn-O based oxide sintered body can be produced which can be used in applications such as barrier films and protective films.

此時,於本發明之另一樣態中,較佳係於燒成步驟中,在大氣中之燒成爐內環境下,以昇溫速度為0.3~1.0℃/min昇溫至1300℃以上1400℃以下、15小時以上25小時以內之條件,來將前述成形體進行燒成。At this time, in another aspect of the present invention, it is preferable that the temperature is raised to 1300 ° C or higher and 1400 ° C or lower at a heating rate of 0.3 to 1.0 ° C / min under a firing furnace atmosphere in the atmosphere in the firing step. The formed body is fired under conditions of 15 hours to 25 hours.

藉由以上述條件進行成形體之燒成,而可製造更高密度且低電阻的Sn-Zn-O系氧化物燒結體。 [發明效果]By firing the molded body under the above conditions, a Sn-Zn-O-based oxide sintered body with higher density and low resistance can be produced. [Inventive effect]

依據本發明,成為可作為可使用於阻隔膜或保護膜等之用途中,高密度且低電阻的Sn-Zn-O系氧化物燒結體。According to the present invention, it becomes a Sn-Zn-O-based oxide sintered body which can be used as a barrier film, a protective film, or the like with high density and low resistance.

以下,針對本發明之Sn-Zn-O系氧化物燒結體及其製造方法,一邊參照附圖一邊依以下順序進行說明。另外,本發明並不限定於以下之例,在不脫離本發明之要旨的範圍內可任意地變更。   1.Sn-Zn-O系氧化物燒結體   2.Sn-Zn-O系氧化物燒結體之製造方法    2-1.造粒步驟    2-2.成形步驟    2-3.燒成步驟Hereinafter, the Sn-Zn-O-based oxide sintered body and the method for producing the same according to the present invention will be described in the following order with reference to the drawings. The present invention is not limited to the following examples, and can be arbitrarily changed without departing from the gist of the present invention. 1.Sn-Zn-O based oxide sintered body 2.Sn-Zn-O based oxide sintered body manufacturing method 2-1. Granulation step 2-2. Molding step 2-3. Sintering step

<1.Sn-Zn-O系氧化物燒結體>   首先,針對本發明之Sn-Zn-O系氧化物燒結體來進行說明。本發明之一實施形態之Sn-Zn-O系氧化物燒結體係以作為原子數比Sn/(Sn+Zn)為0.1以上0.3以下之比例包含Sn,以作為相對於全金屬元素之總量之原子數比Ge/(Sn+Zn+Ge+Ta+ Ga)為0.0005以上0.01以下之比例包含第1添加元素Ge,且以作為相對於全金屬元素之總量之原子數比Ta/(Sn+Zn+Ge +Ta+Ga)為0.0005以上0.01以下之比例含有第2添加元素Ta,並且以作為相對於全金屬元素之總量之原子數比Ga/(Sn+Zn+Ge+Ta+Ga)為0.001以上0.1以下之比例含有第3添加元素Ga。如此之本發明之一實施形態之Sn-Zn-O系氧化物燒結體係比電阻為5Ω・cm以上12000Ω・cm以下,相對密度為94%以上。<1. Sn-Zn-O-based oxide sintered body> First, the Sn-Zn-O-based oxide sintered body of the present invention will be described. The Sn-Zn-O-based oxide sintering system according to an embodiment of the present invention contains Sn as a ratio of the atomic ratio Sn / (Sn + Zn) of 0.1 or more and 0.3 or less, as a total amount relative to the total metal element. The ratio of the number of atoms Ge / (Sn + Zn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less. The first additive element Ge is included, and the ratio of the number of atoms to the total metal elements is Ta / (Sn + Zn + Ge + Ta + Ga) contains 0.002 or more and 0.01 or less and contains the second additive element Ta, and the atomic ratio Ga / (Sn + Zn + Ge + Ta + Ga) as the total amount of the total metal elements is given by The third additive element Ga is contained at a ratio of 0.001 to 0.1. As such, the specific resistance of the Sn-Zn-O-based oxide sintering system according to one embodiment of the present invention is 5 Ω ・ cm or more and 12000 Ω ・ cm or less, and the relative density is 94% or more.

作為本發明之一實施形態之Sn-Zn-O系氧化物燒結體之主原料的氧化錫及氧化鋅係將僅為氧化鋅錫化合物,或是包含氧化錫與氧化鋅之混合粉的原料粉末,以作為原子數比Sn/(Sn+Zn)為0.1以上0.3以下之比例含有Sn。Tin oxide and zinc oxide which are the main raw materials of the Sn-Zn-O based oxide sintered body according to an embodiment of the present invention will be only zinc oxide tin compounds, or raw material powders containing a mixed powder of tin oxide and zinc oxide. Sn is contained in such a proportion that the atomic ratio Sn / (Sn + Zn) is 0.1 or more and 0.3 or less.

因Sn之含量,而於燒結後之燒結體的結晶構造觀察到差異。在以作為原子數比Sn/(Sn+Zn)為0.1以上0.3以下之比例含有Sn的情況,纖鋅礦型結晶構造之ZnO相與尖晶石型結晶構造之Zn2 SnO4 相成為主成分。在以超過0.3、0.9以下之比例包含的情況,尖晶石型結晶構造之Zn2 SnO4 相與金紅石型結晶構造之SnO2 相成為主成分。若金紅石型結晶構造之SnO2 相之主成分增加,則成為電阻值之上昇。又,透過率亦會下降。Due to the Sn content, a difference was observed in the crystal structure of the sintered body after sintering. When Sn is contained at a ratio of Sn / (Sn + Zn) of 0.1 to 0.3, the ZnO phase of the wurtzite crystal structure and the Zn 2 SnO 4 phase of the spinel crystal structure become the main components . In a case where the ratio exceeds 0.3, 0.9 or less contained, Zn spinel type crystal structure of SnO 2 SnO 4 phase and a rutile type crystal structure mainly composed of 2 complementary. When the main component of the SnO 2 phase of the rutile crystal structure increases, the resistance value increases. Also, the transmittance will decrease.

原子數比Sn/(Sn+Zn),更佳為0.16以上0.23以下。若為此範圍,則成為所期望之電阻值,又,針對密度亦成為98%以上,而更佳。The atomic ratio Sn / (Sn + Zn) is more preferably 0.16 to 0.23. In this range, the desired resistance value is obtained, and the density is preferably 98% or more, which is more preferable.

在製造Sn-Zn-O系氧化物燒結體時,如前述般地,於燒結時,從1100℃附近起開始生成Zn2 SnO4 化合物,超過1400℃後Zn之揮發開始,1450℃附近起Zn之揮發變得明顯。若為了提昇Sn-Zn-O系氧化物燒結體的密度而以高溫進行燒成,則由於Zn之揮發進行,因此粒界擴散或粒彼此之結合為弱,而無法得到高密度之氧化物燒結體。另一方面,針對導電性,由於Zn2 SnO4 、ZnO、SnO2 為缺乏導電性的物質,因此即使調整摻合比來調整化合物相或ZnO、SnO2 的量,亦無法將導電性大幅地改善。When manufacturing a Sn-Zn-O-based oxide sintered body, as described above, during sintering, Zn 2 SnO 4 compounds start to be formed from around 1100 ° C, and the volatilization of Zn begins to exceed 1400 ° C, and Zn starts from around 1450 ° C. The volatility becomes apparent. If the firing is performed at a high temperature in order to increase the density of the Sn-Zn-O-based oxide sintered body, the volatilization of Zn progresses, so the grain boundary diffusion or the combination of grains is weak, and high density oxide sintering cannot be obtained. body. On the other hand, regarding conductivity, since Zn 2 SnO 4 , ZnO, and SnO 2 are substances lacking conductivity, even if the blending ratio is adjusted to adjust the amount of the compound phase or the amount of ZnO and SnO 2 , the conductivity cannot be greatly increased. improve.

(添加元素)   因此,於本發明中,為了改善上述導電性而添加第1至第3添加元素。亦即,藉由添加鍺(Ge)作為第1添加元素、鉭(Ta)作為第2添加元素、並且鎵(Ga)作為第3添加元素,而成為可得到高密度且低電阻的Sn-Zn-O系氧化物燒結體。(Additive element) Therefore, in the present invention, in order to improve the above-mentioned conductivity, the first to third additive elements are added. That is, by adding germanium (Ge) as the first additive element, tantalum (Ta) as the second additive element, and gallium (Ga) as the third additive element, high density and low resistance Sn-Zn can be obtained. -O-based oxide sintered body.

[第1添加元素]   為了氧化物燒結體之緻密化,藉由添加第1添加元素Ge,而成為可得到高密度化之效果。第1添加元素Ge係促進粒界擴散,並幫助粒彼此之晶頸生長,使粒彼此之結合成為強固,而有助於緻密化。在此,將第1添加元素Ge相對於全金屬元素之總量的原子數比Ge/(Sn+Zn+Ge+Ta+Ga)設為0.0005以上0.01以下的原因在於,在上述原子數比Ge/ (Sn+Zn+Ge+Ta+Ga)為未達0.0005的情況,無法展現高密度化的效果之故(參照比較例10)。在上述原子數比Ge/(Sn+ Zn+Ge+Ta+Ga)為超過0.01的情況,亦無法展現高密度化的效果(參照比較例9)。且會生成其他化合物,例如Zn2 Ge3 O8 之化合物之故。[First Additive Element] In order to densify the oxide sintered body, the effect of high density can be obtained by adding the first additive element Ge. The first additive element, Ge, promotes grain boundary diffusion, and helps the crystal necks of the grains grow, so that the grains are strongly bonded to each other, thereby contributing to densification. Here, the reason why the atomic ratio Ge / (Sn + Zn + Ge + Ta + Ga) of the first additive element Ge to the total metal element is set to 0.0005 or more and 0.01 or less is because the atomic ratio Ge When (Sn + Zn + Ge + Ta + Ga) is less than 0.0005, the effect of high density cannot be exhibited (see Comparative Example 10). Even when the atomic ratio Ge / (Sn + Zn + Ge + Ta + Ga) exceeds 0.01, the effect of high density cannot be exhibited (see Comparative Example 9). And other compounds, such as Zn 2 Ge 3 O 8 compounds, are formed.

然而,於僅添加有第1添加元素之Ge時,氧化物燒結體之密度雖會提昇,但導電性並未獲得改善。However, when only the first additive element Ge is added, although the density of the oxide sintered body is increased, the conductivity is not improved.

[第2添加元素]   在以作為原子數比Sn/(Sn+Zn)為0.1以上0.3以下之比例含有Sn的條件下,添加有上述第1添加元素Ge的Sn-Zn-O系氧化物燒結體係如上述般地密度雖提昇但於導電性留有課題。[Second additive element] 烧结 Sn-Zn-O-based oxide to which the first additive element Ge is added is sintered under the condition that Sn is contained in a ratio of Sn / (Sn + Zn) of 0.1 to 0.3 in terms of atomic ratio. Although the density of the system is increased as described above, there is a problem in the conductivity.

因此,添加第2添加元素Ta。藉由第2添加元素Ta之添加而在維持氧化物燒結體之高密度的狀態下導電性獲得改善。另外,第2添加元素Ta為5價以上之元素。Therefore, the second addition element Ta is added. The addition of the second additive element Ta improves the conductivity while maintaining the high density of the oxide sintered body. The second additive element Ta is an element having a valence of 5 or more.

添加之量,必須使第2添加元素Ta相對於全金屬元素之總量的原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.0005以上0.01以下。在上述原子數比Ta/(Sn+Zn+Ge+Ta+ Ga)為未達0.0005的情況,導電性無法提高(參照比較例12)。另一方面,在上述原子數比Ta/(Sn+Zn+Ge+Ta+Ga)為超過0.01的情況,由於會生成其他之化合物相,例如Ta2 O5 、ZnTa2 O6 等之化合物相,因此會使導電性惡化(參照比較例11)。The amount of addition must be such that the atomic ratio Ta / (Sn + Zn + Ge + Ta + Ga) of the second additive element Ta to the total metal element is 0.0005 or more and 0.01 or less. When the atomic ratio Ta / (Sn + Zn + Ge + Ta + Ga) is less than 0.0005, the conductivity cannot be improved (see Comparative Example 12). On the other hand, when the atomic ratio Ta / (Sn + Zn + Ge + Ta + Ga) exceeds 0.01, other compound phases such as compound phases such as Ta 2 O 5 and ZnTa 2 O 6 are generated. Therefore, the conductivity is deteriorated (see Comparative Example 11).

[第3添加元素]   如上述般,藉由第2添加元素Ta之添加而導電性獲得改善。然而,Ta會與Zn2 SnO4 相中之Sn、SnO2 置換來進行固溶,因此,有時無法得到電阻值為所期望之導電性。[Third Additive Element] As described above, the addition of the second additive element Ta improves the conductivity. However, Ta is replaced with Sn and SnO 2 in the Zn 2 SnO 4 phase to perform solid solution. Therefore, the desired conductivity may not be obtained in some cases.

因此,添加第3添加元素Ga。藉由添加第3添加元素Ga,而有望對於Zn、Zn2 SnO4 相中之Zn的導電性之改善。Therefore, the third addition element Ga is added. The addition of the third additive element Ga is expected to improve the conductivity of Zn in the Zn and Zn 2 SnO 4 phases.

添加之量,必須使第3添加元素Ge相對於全金屬元素之總量的原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.001以上0.1以下。在上述原子數比Ga/(Sn+Zn+Ge+Ta+ Ga)為未達0.001的情況,導電性無法提高。(參照比較例14)。另一方面,在上述原子數比Ga/(Sn+Zn+Ge+Ta+Ga)為超過0.1的情況,由於會生成其他之化合物相,例如Ga2 O3 等之化合物相,因此會使導電性惡化(參照比較例13)。The amount of addition must be such that the atomic ratio Ge / (Sn + Zn + Ge + Ta + Ga) of the third additive element Ge to the total metal element is 0.001 or more and 0.1 or less. When the atomic ratio Ga / (Sn + Zn + Ge + Ta + Ga) is less than 0.001, the conductivity cannot be improved. (Refer to Comparative Example 14). On the other hand, when the above-mentioned atomic ratio Ga / (Sn + Zn + Ge + Ta + Ga) exceeds 0.1, other compound phases such as a compound phase such as Ga 2 O 3 may be formed, and thus conductive. Sexual deterioration (see Comparative Example 13).

另外,只要不損害作為本發明之一實施形態之Sn-Zn-O系氧化物燒結體的特徵之可使用於阻隔膜或保護膜等之用途中,高密度(相對密度為94%以上)且低電阻(比電阻為5Ω・cm以上12000Ω・cm以下)的性質者,則亦可進一步包含添加元素。作為進一步之添加元素係可列舉例如:Si、Ti、Bi、Ce、Al、Nb、W、Mo等。In addition, as long as the characteristics of the Sn-Zn-O-based oxide sintered body as one embodiment of the present invention are not impaired, it can be used in applications such as barrier films or protective films, and has a high density (relative density of 94% or more) and Those having low resistance (specific resistance is 5 Ω ・ cm or more and 12000 Ω ・ cm or less) may further include an additive element. Examples of further additional element systems include Si, Ti, Bi, Ce, Al, Nb, W, Mo, and the like.

(X射線繞射峰值)   於本發明之一實施形態之Sn-Zn-O系氧化物燒結體中,在原子數比Sn/(Sn+Zn)為0.1以上0.3以下時,纖鋅礦型結晶構造之ZnO相與尖晶石型結晶構造之Zn2 SnO4 相成為主成分,又,適當量之第1添加元素Ge與第2添加元素Ta、第3添加元素Ga會與ZnO相中之Zn、Zn2 SnO4 相中之Zn或Sn、SnO2 相中之Sn置換來進行固溶,因此,纖鋅礦型結晶構造之ZnO相、尖晶石型結晶構造之Zn2 SnO4 相以外的其他化合物相不會形成。(X-ray diffraction peak) In the Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention, when the atomic ratio Sn / (Sn + Zn) is 0.1 or more and 0.3 or less, wurtzite-type crystals The ZnO phase of the structure and the Zn 2 SnO 4 phase of the spinel-type crystal structure become the main components. In addition, appropriate amounts of the first additive element Ge, the second additive element Ta, and the third additive element Ga will interact with Zn in the ZnO phase. Zn or Sn in the Zn 2 SnO 4 phase and Sn in the SnO 2 phase for solid solution replacement. Therefore, ZnO phase with wurtzite type crystal structure and Zn 2 SnO 4 phase with spinel type crystal structure. No other compound phases will form.

(比電阻)   本發明之一實施形態之Sn-Zn-O系氧化物燒結體的比電阻為5Ω・cm以上12000Ω・cm以下。如上述般地,Sn-Zn-O之氧化物燒結體之比電阻,以往1×106 Ω・cm以上為非常高的比電阻值。於本發明中,藉由摻合Ge、Ta及Ga作為第1~第3添加元素,而使比電阻值降低。(Specific resistance) The specific resistance of the Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention is 5 Ω ・ cm or more and 12000 Ω ・ cm or less. As described above, the specific resistance of the oxide sintered body of Sn—Zn—O has a specific resistance value of 1 × 10 6 Ω 为 cm or more in the past. In the present invention, the specific resistance value is reduced by doping Ge, Ta, and Ga as the first to third additive elements.

以往所使用之ITO的燒結體之比電阻值為2~3×10-4 Ω・cm,藉由以此燒結體作為靶材來進行濺鍍而適宜使用作為液晶或太陽能電子等之透明導電膜。使用本發明之一實施形態之Sn-Zn-O系氧化物燒結體來進行濺鍍所得之透明導電膜係比電阻為10Ω・cm~1×104 Ω・cm左右者,因此,導電性雖比ITO差,但可使用於氣體阻隔膜、水蒸氣阻隔膜等之阻隔膜或保護以避免損傷或衝擊之保護膜等的用途中。本發明之一實施形態之Sn-Zn-O之氧化物燒結體係適於比電阻為10Ω・cm~1×104 Ω・cm左右之膜的濺鍍之比電阻。The sintered body of ITO used in the past has a specific resistance value of 2 to 3 × 10 -4 Ω ・ cm. The sintered body is used as a target for sputtering, and it is suitable to be used as a transparent conductive film for liquid crystal or solar electronics. . A transparent conductive film obtained by sputtering using a Sn-Zn-O oxide sintered body according to an embodiment of the present invention has a specific resistance of about 10 Ω ・ cm to 1 × 10 4 Ω ・ cm. It is inferior to ITO, but can be used in applications such as gas barrier films, water vapor barrier films, or barrier films that protect against damage or impact. The oxide sintering system of Sn-Zn-O according to one embodiment of the present invention is suitable for the specific resistance of sputtering of a film having a specific resistance of about 10 Ω ・ cm to 1 × 10 4 Ω ・ cm.

濺鍍之膜的比電阻值亦會受到濺鍍時之成膜條件,尤其是濺鍍時之氧濃度影響。但,若考慮濺鍍時之生產性、膜之均勻性等,則以膜之比電阻值與結晶體之比電阻值一致為佳。The specific resistance value of the sputtered film will also be affected by the film formation conditions during sputtering, especially the oxygen concentration during sputtering. However, if the productivity during sputtering, the uniformity of the film, and the like are considered, it is preferable that the specific resistance value of the film is consistent with the specific resistance value of the crystal.

又,比電阻值係取決於濺鍍時之成膜速度,因此,比電阻值係越小越好。本發明之一實施形態之Sn-Zn-O系氧化物燒結體的比電阻為5Ω・cm以上12000Ω・cm以下,因此,成為適於濺鍍之氧化物燒結體。在比電阻為未達5Ω・cm的情況,由於所得之膜的電阻值會變低,因此發生來自附近之電極的洩漏一事成為問題。又,若比電阻值為超過12000Ω・cm,則變得難以進行放電,針對直流濺鍍無法安定地進行成膜,因此成為問題。Since the specific resistance value depends on the film formation speed during sputtering, the smaller the specific resistance value, the better. Since the specific resistance of the Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention is 5 Ω ・ cm or more and 12000 Ω ・ cm or less, it is an oxide sintered body suitable for sputtering. In the case where the specific resistance is less than 5 Ω 由于 cm, the resistance value of the obtained film becomes low, so that leakage from a nearby electrode becomes a problem. In addition, if the specific resistance value exceeds 12000 Ω ・ cm, it becomes difficult to perform discharge, and film formation cannot be performed stably with respect to DC sputtering, which is a problem.

進而,於本發明之一實施形態中,藉由使金屬原子數比成為Sn/(Zn+Sn)為0.16以上0.23以下,而比電阻值係可設為5Ω・cm以上110Ω・cm以下之範圍(參照實施例1、8、9)。藉由使比電阻值成為5Ω・cm以上110Ω・cm以下,而提昇成膜速度,而更佳。Furthermore, in one embodiment of the present invention, by setting the metal atomic ratio to Sn / (Zn + Sn) to be 0.16 or more and 0.23 or less, the specific resistance value can be set to a range of 5Ω ・ cm to 110Ω ・ cm. (Refer to Examples 1, 8, and 9). By setting the specific resistance value to be 5 Ω ・ cm or more and 110 Ω ・ cm or less, the film formation speed is increased, and it is more preferable.

(相對密度)   本發明之一實施形態之Sn-Zn-O系氧化物燒結體的相對密度為94%以上。如專利文獻1所示般,於以作為原子數比Sn/(Sn+Zn)為0.23以上0.5以下之比率摻合而成的Sn-Zn-O之氧化物燒結體中,相對密度係因燒結時之Zn的揮發而無法得到相對密度高的結晶體。於本發明中,藉由以特定量摻合上述之添加元素,而可提昇相對密度。(Relative density) The relative density of the Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention is 94% or more. As shown in Patent Document 1, in an oxide sintered body of Sn-Zn-O blended at a ratio of Sn / (Sn + Zn) of 0.23 to 0.5, the relative density is due to sintering. When Zn is volatilized, crystals with high relative density cannot be obtained. In the present invention, the relative density can be increased by blending the aforementioned additional elements in a specific amount.

另外,藉由使金屬原子數比Sn/(Zn+Sn)成為0.16以上0.23以下,而可使前述相對密度提昇為98%以上。在相對密度為98%以上的情況,靶材強度提昇而濺鍍時之成膜速度提昇,同時起因於靶材之釋氣變少,而成為可安定的成膜。The relative density can be increased to 98% or more by setting the metal atomic ratio Sn / (Zn + Sn) to 0.16 or more and 0.23 or less. When the relative density is 98% or more, the strength of the target is increased and the film formation speed during sputtering is increased. At the same time, the outgassing of the target is reduced, and it becomes a stable film formation.

<2.Sn-Zn-O系氧化物燒結體之製造方法>   接著,針對本發明之Sn-Zn-O系氧化物燒結體之製造方法來進行說明。本發明之一實施形態係具有鋅(Zn)與錫(Sn)作為成分之Sn-Zn-O系氧化物燒結體之製造方法,其中,具有下列步驟:將鋅之氧化物粉末、錫之氧化物粉末、及含有添加元素之氧化物粉末進行混合而製作造粒粉末的造粒步驟S1;將前述造粒粉末進行加壓成形而得到成形體的成形步驟S2;以及將前述成形體進行燒成而得到氧化物燒結體的燒成步驟S3。例如,本發明之一實施形態之Sn-Zn-O系氧化物燒結體係於僅為氧化鋅錫化合物,或是包含氧化錫與氧化鋅之混合粉的原料粉末中,以特定的比率摻合第1添加元素之氧化鍺、第2添加元素之氧化鉭、第3添加元素之氧化鎵,進行造粒,並將造粒粉以冷均壓等而成形,將該成形體以燒成爐進行燒成,而得到燒結體。以下,針對各步驟,個別地進行說明。<2. Manufacturing method of Sn-Zn-O-based oxide sintered body> Next, the manufacturing method of the Sn-Zn-O-based oxide sintered body of the present invention will be described. An embodiment of the present invention is a method for producing a sintered body of Sn-Zn-O oxide having zinc (Zn) and tin (Sn) as components, which includes the following steps: oxidizing zinc oxide powder and tin A granulation step S1 for preparing a granulated powder by mixing an object powder and an oxide powder containing an additive element; a forming step S2 in which the granulated powder is pressure-molded to obtain a formed body; and the formed body is fired Then, a firing step S3 of the oxide sintered body is obtained. For example, the Sn-Zn-O oxide sintering system according to an embodiment of the present invention is blended with a specific ratio of raw material powder containing only zinc tin oxide compounds or mixed powders of tin oxide and zinc oxide. Germanium oxide with 1 added element, tantalum oxide with 2nd added element, and gallium oxide with 3rd added element are granulated, and the granulated powder is formed by cold equal pressure, etc., and the formed body is fired in a firing furnace. To obtain a sintered body. Hereinafter, each step will be described individually.

(2-1.造粒步驟)   首先,於造粒步驟S1中,準備主原料。成為主原料的氧化錫及氧化鋅係將僅為氧化鋅錫化合物,或是包含氧化錫與氧化鋅之混合粉的原料粉末,以作為原子數比Sn/ (Sn+Zn)為0.1以上0.3以下之比例含有Sn。主原料係使用有氧化錫與氧化鋅之混合粉者較可容易調整摻合比,而為佳。例如,此原料粉末係為SnO2 粉與ZnO粉。又,準備含有第1添加元素至第3添加元素的氧化物,添加於此主原料中進行調配。例如,準備作為第1添加元素Ge之GeO2 粉,及作為第2添加元素Ta之Ta2 O5 粉,作為第3添加元素Ga之Ga2 O3 粉,添加於主原料中進行調配。(2-1. Granulation step) First, in a granulation step S1, a main raw material is prepared. The tin oxide and zinc oxide system that will be the main raw materials will be only zinc tin oxide compounds, or raw material powders containing mixed powders of tin oxide and zinc oxide, with an atomic ratio Sn / (Sn + Zn) of 0.1 to 0.3. The ratio contains Sn. The main raw material is preferably a mixed powder of tin oxide and zinc oxide, which can be easily adjusted. For example, the raw material powders are SnO 2 powder and ZnO powder. In addition, an oxide containing the first additive element to the third additive element is prepared and added to the main raw material to prepare it. For example, a GeO 2 powder as the first additive element Ge and a Ta 2 O 5 powder as the second additive element Ta and a Ga 2 O 3 powder as the third additive element Ga are prepared and added to the main raw material for blending.

於造粒步驟S1中,以使金屬原子數比成為Sn/(Zn+Sn)為0.1以上0.3以下、Ge/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、Ta/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、Ga/(Zn+Sn+Ge+Ta+Ga)為0.001以上0.1以下的方式來將鋅之氧化物粉末、錫之氧化物粉末、及含有添加元素之氧化物粉末進行混合。如此般,以使Sn/(Zn+Sn)成為0.1以上0.3以下的比例,且如上述般,作為添加元素而將鍺(Ge)、鉭(Ta)、及鎵(Ga)3種以特定的比例進行混合,藉此而可製造可使用於阻隔膜或保護膜等之用途中,高密度且低電阻的Sn-Zn-O系氧化物燒結體。In the granulation step S1, the metal atomic ratio is set such that Sn / (Zn + Sn) is 0.1 or more and 0.3 or less, Ge / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less, and Ta / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less, and Ga / (Zn + Sn + Ge + Ta + Ga) is 0.001 or more and 0.1 or less, so that zinc oxide powder, tin oxide powder, and The oxide powder containing the additive element is mixed. In this manner, the three kinds of germanium (Ge), tantalum (Ta), and gallium (Ga) are specified as the additive elements so that Sn / (Zn + Sn) becomes a ratio of 0.1 to 0.3, as described above. By mixing the ratios, a Sn-Zn-O-based oxide sintered body having a high density and a low resistance, which can be used in applications such as a barrier film or a protective film, can be produced.

接著,將所調配的原料粉末與純水或超純水、有機黏合劑、分散劑、消泡劑以使原料粉末濃度成為特定之濃度的方式於混合槽中進行混合。並且,使用投入有硬質ZrO2 球的珠磨裝置等,將原料粉末進行濕式粉碎之後,進行混合攪拌而得到漿體。藉由將所得之漿體以噴霧乾燥裝置等進行噴霧及乾燥,而可得到造粒粉末。Next, the prepared raw material powder and pure water or ultrapure water, an organic binder, a dispersant, and an antifoaming agent are mixed in a mixing tank so that the concentration of the raw material powder becomes a specific concentration. Then, the raw material powder is wet-pulverized using a bead mill or the like in which hard ZrO 2 balls are put, and then mixed and stirred to obtain a slurry. A granulated powder can be obtained by spraying and drying the obtained slurry with a spray-drying device or the like.

(2-2.成形步驟)   成形步驟S2係將造粒步驟S1中所得之造粒粉末進行加壓成形,而得到成形體的步驟。於成形步驟S2中,為了去除造粒粉之粒子間的空孔,例如,以294MPa(3.0ton/cm2 )左右的壓力進行加壓成形。針對加壓成形之方法雖無特別限定,但例如,較佳係將造粒步驟S1中所得之造粒粉末填充於橡膠模,並使用可施加高壓力的冷均壓(CIP:Cold Isostatic Press)。(2-2. Molding step) The molding step S2 is a step of press-molding the granulated powder obtained in the granulation step S1 to obtain a compact. In the forming step S2, in order to remove voids between the particles of the granulated powder, for example, pressure forming is performed at a pressure of about 294 MPa (3.0 ton / cm 2 ). Although the method for pressure forming is not particularly limited, for example, it is preferable that a rubber mold is filled with the granulated powder obtained in the granulation step S1, and a cold equalizing pressure (CIP: Cold Isostatic Press) capable of applying high pressure is preferably used. .

(2-3.燒成步驟)   燒成步驟S3係於燒成爐內之特定的昇溫速度中,以特定的溫度且特定的時間之條件,將上述成形步驟S2中所得之成形體進行燒成,而得到燒結體的步驟。燒成步驟S3,例如,係於大氣中之燒成爐內環境中進行。於本發明之一實施形態之Sn-Zn-O系氧化物燒結體之製造方法中,於該等之燒成條件上亦具有特徵,以下詳細地進行說明。(2-3. Firing step) (1) The firing step S3 is based on a specific temperature rise rate in the firing furnace, and fires the formed body obtained in the above-mentioned forming step S2 under the conditions of a specific temperature and a specific time. , And the step of obtaining a sintered body. The firing step S3 is performed, for example, in an atmosphere inside a firing furnace. The method for producing a Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention is also characterized by these firing conditions, and will be described in detail below.

[昇溫速度]   於燒結爐內之從700℃至特定的燒結溫度為止之昇溫速度,較佳係於0.3~1.0℃/min之速度中,將成形體進行燒成。其係具有促進ZnO、SnO2 或Zn2 SnO4 化合物之擴散,提昇燒結性,並且提昇導電性的效果之故。又,藉由設為如此之昇溫速度,亦具有於高溫域中抑制ZnO或Zn2 SnO4 之揮發的效果。[Heating rate] The heating rate in the sintering furnace from 700 ° C to a specific sintering temperature is preferably at a rate of 0.3 to 1.0 ° C / min, and the molded body is fired. It has the effect of promoting the diffusion of ZnO, SnO 2 or Zn 2 SnO 4 compounds, improving sinterability, and improving conductivity. Moreover, by setting such a temperature increase rate, it is also effective in suppressing volatilization of ZnO or Zn 2 SnO 4 in a high temperature region.

另外,於本發明之一實施形態之Sn-Zn-O系氧化物燒結體之製造方法中,SnO2 亦有於燒結中(較低的溫度域)存在的情況,但,Sn/(Zn+Sn)為0.1以上0.3以下,若指定之溫度燒結結束,則SnO2 相會消失,而以X射線繞射分析變得不能測定SnO2 相之繞射峰值。In addition, in the method for manufacturing a Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention, SnO 2 may be present during sintering (lower temperature range). However, Sn / (Zn + Sn) is 0.1 or more and 0.3 or less. When the sintering at the specified temperature is completed, the SnO 2 phase disappears, and the diffraction peak of the SnO 2 phase cannot be measured by X-ray diffraction analysis.

在燒結爐內之昇溫速度為未達0.3℃/min的情況中,化合物之擴散會衰退。又,在超過1.0℃/min的情況,由於昇溫速度迅速,因此化合物形成會不完全,而無法製作緻密的燒結體。(參照比較例3、4)。In the case where the temperature rise rate in the sintering furnace is less than 0.3 ° C / min, the diffusion of the compound will decline. When the temperature exceeds 1.0 ° C./min, the temperature rise rate is rapid, so that the formation of the compound is incomplete, and a dense sintered body cannot be produced. (See Comparative Examples 3 and 4).

[燒結溫度]   燒結溫度較佳係設為1300℃以上1400℃以下。在燒結溫度為未達1300℃的情況(參照比較例5),溫度會過低,而ZnO、SnO2 、Zn2 SnO4 化合物中之燒結的粒界擴散不進行。另一方面,即使是在超過1400℃的情況(參照比較例6),雖粒界擴散被促進而燒結進行,但無法抑制Zn成分之揮發,而導致於燒結體內部殘留大量空孔。[Sintering temperature] The sintering temperature is preferably set to 1300 ° C or higher and 1400 ° C or lower. When the sintering temperature is less than 1300 ° C (see Comparative Example 5), the temperature is too low, and the sintered grain boundary diffusion in the ZnO, SnO 2 , and Zn 2 SnO 4 compounds does not proceed. On the other hand, even when the temperature exceeds 1400 ° C (see Comparative Example 6), although grain boundary diffusion is promoted and sintering proceeds, the volatilization of the Zn component cannot be suppressed, and a large number of voids remain in the sintered body.

[保持時間]   保持時間較佳係設為15小時以上25小時以內。若低於15小時,則燒結會不完全,因此,成為變形或翹曲大的燒結體,並且粒界擴散不進行,而燒結不進行。其結果,無法製作緻密的燒結體(參照比較例7)。另一方面,在超過25小時的情況,ZnO或Zn2 SnO4 之揮發會變多,而造成密度的降低或作業效率的惡化、及成本高之結果(參照比較例8)。[Hold time] The hold time is preferably set to 15 hours or more and 25 hours or less. If it is less than 15 hours, the sintering will be incomplete. Therefore, the sintered body will be deformed or warped, and the grain boundary diffusion will not proceed, and the sintering will not proceed. As a result, a dense sintered body cannot be produced (see Comparative Example 7). On the other hand, when it exceeds 25 hours, the volatilization of ZnO or Zn 2 SnO 4 increases, which results in a decrease in density, deterioration in work efficiency, and high cost (see Comparative Example 8).

以如此之條件所得之以Zn及Sn作為主成分的本發明之一實施形態之Sn-Zn-O系氧化物燒結體,由於導電性亦獲得改善,因此成為可以DC濺鍍之成膜。又,由於未使用特別的製造方法,因此亦可應用於圓筒形靶材。 [實施例]The Sn-Zn-O-based oxide sintered body according to one embodiment of the present invention, which has Zn and Sn as main components, obtained under such conditions, has improved conductivity, and is therefore a film capable of DC sputtering. Moreover, since no special manufacturing method is used, it can also be applied to a cylindrical target. [Example]

以下,針對本發明,使用實施例來進一步具體地說明,但,本發明不受以下之實施例任何限定。Hereinafter, the present invention will be described in more detail using examples. However, the present invention is not limited to the following examples.

(實施例1)   於實施例1中,準備SnO2 粉、ZnO粉、作為第1添加元素Ge之GeO2 粉、作為第2添加元素Ta之Ta2 O5 粉、以及作為第3添加元素Ga之Ga2 O3 粉。(Example 1) In Example 1, a SnO 2 powder, a ZnO powder, a GeO 2 powder as a first additive element Ge, a Ta 2 O 5 powder as a second additive element Ta, and a Ga as a third additive element were prepared. Ga 2 O 3 powder.

接著,以使Sn與Zn之原子數比Sn/(Sn+Zn)成為0.2的方式來調配SnO2 粉與ZnO粉,以使第1添加元素Ge之原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.004、使第2添加元素Ta之原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.002、及使第3添加元素Ga之原子數比Ga/((Sn+Zn+Ge+Ta+Ga)成為0.02的方式來調配GeO2 粉、Ta2 O5 粉、及Ga2 O3 粉。Next, the SnO 2 powder and ZnO powder are blended so that the atomic ratio of Sn and Zn Sn / (Sn + Zn) is 0.2, so that the atomic number ratio of the first additive element Ge is Ge / (Sn + Zn + Ge + Ta + Ga) is 0.004, the atomic ratio of the second additive element Ta is Ta / (Sn + Zn + Ge + Ta + Ga) is 0.002, and the atomic ratio of the third additive element Ga is Ga / ((Sn + Zn + Ge + Ta + Ga) was adjusted to 0.02 to mix GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder.

接著,將所調配的原料粉末與純水或超純水、有機黏合劑、分散劑、消泡劑以使原料粉末濃度成為55~65質量%的方式於混合槽中進行混合。接著,使用投入有硬質ZrO2 球的珠磨裝置(Ashizawa Finetech股份有限公司製,LMZ型),進行濕式粉碎直至原料粉末之平均粒徑成為1μm以下之後,進行10小時以上混合攪拌而得到漿體。另外,為了測定原料粉末之平均粒徑係使用有雷射繞射式粒度分布測定裝置(島津製作所製,SALD-2200)。Next, the prepared raw material powder and pure water or ultrapure water, an organic binder, a dispersant, and an antifoaming agent are mixed in a mixing tank so that the concentration of the raw material powder becomes 55 to 65% by mass. Next, using a bead mill device (type LMZ, manufactured by Ashizawa Finetech Co., Ltd.) with hard ZrO 2 balls, wet grinding was performed until the average particle diameter of the raw material powder became 1 μm or less, and the mixture was stirred for more than 10 hours to obtain a slurry. body. In addition, in order to measure the average particle diameter of the raw material powder, a laser diffraction type particle size distribution measuring device (SALD-2200, manufactured by Shimadzu Corporation) was used.

將所得之漿體以噴霧乾燥裝置(大川原化工機股份有限公司製,ODL-20型)進行噴霧及乾燥,而得到造粒粉。The obtained slurry was spray-dried with a spray-drying device (manufactured by Ogawara Chemical Machinery Co., Ltd., ODL-20 type) to obtain granulated powder.

接著,將所得之造粒粉末填充於橡膠模,以冷均壓施加294MPa(3ton/cm2 )之壓力而成形,將所得之直徑約250mm之成形體投入常壓燒成爐中,於燒結爐內導入空氣直至700℃為止。在確認燒成爐內之溫度成為700℃後,導入氧,昇溫至1350℃,且,以1350℃保持20小時。此時之昇溫速度係設為0.7℃/min。Next, the obtained granulated powder was filled in a rubber mold, and formed by applying a pressure of 294 MPa (3ton / cm 2 ) under cold equalizing pressure, and the formed body having a diameter of about 250 mm was put into a normal-pressure firing furnace, and the sintering furnace was used. Air was introduced into it until 700 ° C. After confirming that the temperature in the firing furnace was 700 ° C, oxygen was introduced, the temperature was raised to 1350 ° C, and the temperature was maintained at 1350 ° C for 20 hours. The temperature increase rate at this time was set to 0.7 ° C / min.

保持時間結束後停止氧導入,進行冷卻,而得到實施例1之Sn-Zn-O系氧化物燒結體。After the holding time was over, the introduction of oxygen was stopped and cooling was performed to obtain a Sn-Zn-O-based oxide sintered body of Example 1.

接著,將實施例1之Sn-Zn-O系氧化物燒結體使用平面磨床與磨削中心(GRINDING CENTER),施行加工成直徑200mm、厚度5mm。Next, the Sn-Zn-O-based oxide sintered body of Example 1 was processed into a diameter of 200 mm and a thickness of 5 mm using a surface grinder and a grinding center.

以阿基米德法測定此加工體的密度之結果,相對密度為99.0%。又,以四探針法測定比電阻之結果為5.5Ω・cm。As a result of measuring the density of this processed body by the Archimedes method, the relative density was 99.0%. The specific resistance measured by the four-probe method was 5.5 Ω ・ cm.

又,將此加工體的一部分切斷,藉由乳缽粉碎而成為粉末。針對此粉末,以使用有CuKα射線之X射線繞射裝置[X’Pert-PRO(PANalytical公司製)]分析的結果,尖晶石型結晶構造之Zn2 SnO4 相為66%、及纖鋅礦型結晶構造之ZnO相為全體的34%繞射,無測定出其他的化合物相之繞射峰值。將該等結果顯示於表1。In addition, a part of this processed body was cut and pulverized by a mortar to obtain a powder. This powder was analyzed using an X-ray diffraction device [X'Pert-PRO (manufactured by PANalytical)] with CuKα rays, and the spinel-type crystal structure had a Zn 2 SnO 4 phase of 66% and fiber zinc. The ZnO phase of the ore-type crystal structure has an overall diffraction of 34%, and the diffraction peaks of other compound phases have not been measured. These results are shown in Table 1.

(實施例2)   於實施例2中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.1之比例進行調配,除此之外,以與實施例1相同方式,而得到實施例2之Sn-Zn-O系氧化物燒結體。與實施例1相同地,進行粉末之X射線繞射分析之結果,纖鋅礦型ZnO相為70%、及尖晶石型結晶構造之Zn2 SnO4 相為30%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為96.0%,比電阻值為1780Ω・cm。將該等結果顯示於表1。(Example 2) In Example 2, the ratio of the atomic ratio of Sn and Zn Sn / (Sn + Zn) was set to 0.1, and other than that, an example was obtained in the same manner as in Example 1. 2 of Sn-Zn-O based oxide sintered body. As a result of X-ray diffraction analysis of the powder as in Example 1, the wurtzite-type ZnO phase was 70% and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 30% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 96.0%, and the specific resistance value was 1780 Ω ・ cm. These results are shown in Table 1.

(實施例3)   於實施例3中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.3之比例進行調配,除此之外,以與實施例1相同方式,而得到實施例3之Sn-Zn-O系氧化物燒結體。與實施例1相同地,進行粉末之X射線繞射分析之結果,纖鋅礦型ZnO相為5%、及尖晶石型結晶構造之Zn2 SnO4 相為95%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為95.5%,比電阻值為7100Ω・cm。將該等結果顯示於表1。(Example 3) In Example 3, blending was performed at a ratio of Sn / Zn atomic ratio Sn / (Sn + Zn) to 0.3. Except that, Example 1 was obtained in the same manner as in Example 1. Sn-Zn-O-based oxide sintered body of 3. As a result of X-ray diffraction analysis of the powder in the same manner as in Example 1, the wurtzite-type ZnO phase was 5%, and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 95% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 95.5%, and the specific resistance was 7100 Ω ・ cm. These results are shown in Table 1.

(實施例4)   於實施例4中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.1之比例進行調配,以使第1添加元素Ge之原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.0005、使第2添加元素Ta之原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.0005、及使第3添加元素Ga之原子數比Ga/(Sn+Zn+Ge+Ta+Ga)成為0.001的方式來調配GeO2 粉、Ta2 O5 粉、及Ga2 O3 粉,除此之外,以與實施例1相同方式,而得到實施例4之Sn-Zn-O系氧化物燒結體。與實施例2相同地,纖鋅礦型ZnO相為70%、及尖晶石型結晶構造之Zn2 SnO4 相為30%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為95.0%,比電阻值為5300Ω・cm。將該等結果顯示於表1。(Example 4) In Example 4, the ratio of the atomic ratio of Sn and Zn Sn / (Sn + Zn) was set to 0.1 so that the atomic ratio of the first additive element Ge was Ge / (Sn + Zn). + Ge + Ta + Ga) is 0.0005, the atomic ratio of the second additive element Ta is Ta / (Sn + Zn + Ge + Ta + Ga) is 0.0005, and the atomic ratio of the third additive element Ga is Ga / ( Sn + Zn + Ge + Ta + Ga) was set to 0.001 to prepare GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder. Except that, the same method as in Example 1 was used to obtain an example. 4 of Sn-Zn-O based oxide sintered body. As in Example 2, the wurtzite-type ZnO phase was 70%, and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 30% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 95.0%, and the specific resistance was 5300 Ω ・ cm. These results are shown in Table 1.

(實施例5)   於實施例5中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.1之比例進行調配,以使第1添加元素Ge之原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.01、使第2添加元素Ta之原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.01、及使第3添加元素Ga之原子數比Ga/(Sn+Zn+Ge+Ta+Ga)成為0.1的方式來調配GeO2 粉、Ta2 O5 粉、及Ga2 O3 粉,除此之外,以與實施例1相同方式,而得到實施例5之Sn-Zn-O系氧化物燒結體。與實施例2相同地,纖鋅礦型ZnO相為70%、及尖晶石型結晶構造之Zn2 SnO4 相為30%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為96.0%,比電阻值為980Ω・cm。將該等結果顯示於表1。Example 5 In Example 5, the ratio of the atomic ratio Sn / (Sn + Zn) of Sn and Zn to 0.1 was adjusted so that the atomic ratio of the first additive element Ge was Ge / (Sn + Zn). + Ge + Ta + Ga) is 0.01, the atomic ratio of the second additive element Ta is Ta / (Sn + Zn + Ge + Ta + Ga) is 0.01, and the atomic ratio of the third additive element Ga is Ga / ( Sn + Zn + Ge + Ta + Ga) was set to 0.1 so that GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder were blended. Except that, Example 1 was obtained in the same manner as in Example 1. 5 of Sn-Zn-O based oxide sintered body. As in Example 2, the wurtzite-type ZnO phase was 70%, and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 30% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 96.0%, and the specific resistance value was 980 Ω980cm. These results are shown in Table 1.

(實施例6)   於實施例6中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.3之比例進行調配,以使第1添加元素Ge之原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.0005、使第2添加元素Ta之原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.0005、及使第3添加元素Ga之原子數比Ga/(Sn+Zn+Ge+Ta+Ga)成為0.001的方式來調配GeO2 粉、Ta2 O5 粉、及Ga2 O3 粉,除此之外,以與實施例1相同方式,而得到實施例6之Sn-Zn-O系氧化物燒結體。與實施例3相同地,纖鋅礦型ZnO相為5%、及尖晶石型結晶構造之Zn2 SnO4 相為95%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為94.7%,比電阻值為10000Ω・cm。將該等結果顯示於表1。(Example 6) In Example 6, the ratio of the atomic ratio Sn / (Sn + Zn) of Sn and Zn to 0.3 was adjusted so that the atomic ratio of the first additive element Ge was Ge / (Sn + Zn). + Ge + Ta + Ga) is 0.0005, the atomic ratio of the second additive element Ta is Ta / (Sn + Zn + Ge + Ta + Ga) is 0.0005, and the atomic ratio of the third additive element Ga is Ga / ( Sn + Zn + Ge + Ta + Ga) was set to 0.001 to prepare GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder. Except that, the same method as in Example 1 was used to obtain an example. Sn-Zn-O-based oxide sintered body of 6. As in Example 3, the wurtzite-type ZnO phase was 5%, and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 95% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 94.7%, and the specific resistance was 10,000 Ω10000cm. These results are shown in Table 1.

(實施例7)   於實施例7中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.3之比例進行調配,以使第1添加元素Ge之原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.01、使第2添加元素Ta之原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.01、及使第3添加元素Ga之原子數比Ga/(Sn+Zn+Ge+Ta+Ga)成為0.1的方式來調配GeO2 粉、Ta2 O5 粉、及Ga2 O3 粉,除此之外,以與實施例1相同方式,而得到實施例7之Sn-Zn-O系氧化物燒結體。與實施例3相同地,纖鋅礦型ZnO相為5%、及尖晶石型結晶構造之Zn2 SnO4 相為95%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為95.0%,比電阻值為9500Ω・cm。將該等結果顯示於表1。(Example 7) In Example 7, the ratio of the atomic ratio Sn / (Sn + Zn) of Sn and Zn to 0.3 was adjusted so that the atomic ratio of the first additive element Ge was Ge / (Sn + Zn). + Ge + Ta + Ga) is 0.01, the atomic ratio of the second additive element Ta is Ta / (Sn + Zn + Ge + Ta + Ga) is 0.01, and the atomic ratio of the third additive element Ga is Ga / ( Sn + Zn + Ge + Ta + Ga) was set to 0.1 so that GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder were blended. Except that, Example 1 was obtained in the same manner as in Example 1. Sn-Zn-O-based oxide sintered body of 7. As in Example 3, the wurtzite-type ZnO phase was 5%, and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 95% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 95.0%, and the specific resistance was 9500 Ω ・ cm. These results are shown in Table 1.

(實施例8)   於實施例8中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.16之比例進行調配,將燒結保持溫度設為1300℃,除此之外,以與實施例1相同方式,而得到實施例8之Sn-Zn-O系氧化物燒結體。與實施例1相同地,進行粉末之X射線繞射分析的結果,尖晶石型結晶構造之Zn2 SnO4 相為54%、及纖鋅礦型結晶構造之ZnO相為全體的46%繞射,無測定出其他的化合物相之繞射峰值。又,相對密度為98.0%,比電阻值為60Ω・cm。將該等結果顯示於表1。(Example 8) In Example 8, the ratio of the atomic ratio of Sn and Zn Sn / (Sn + Zn) was set to 0.16, and the sintering holding temperature was set to 1300 ° C. In the same manner as in Example 1, a Sn-Zn-O-based oxide sintered body of Example 8 was obtained. As a result of X-ray diffraction analysis of the powder as in Example 1, the Zn 2 SnO 4 phase of the spinel type crystal structure was 54%, and the ZnO phase of the wurtzite type crystal structure was 46% The diffraction peaks of other compound phases were not measured. The relative density was 98.0%, and the specific resistance value was 60 Ω ・ cm. These results are shown in Table 1.

(實施例9)   於實施例9中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.23之比例進行調配,將燒結保持溫度設為1400℃,除此之外,以與實施例1相同方式,而得到實施例9之Sn-Zn-O系氧化物燒結體。與實施例1相同地,進行粉末之X射線繞射分析的結果,尖晶石型結晶構造之Zn2 SnO4 相為74%、及纖鋅礦型結晶構造之ZnO相為全體的26%繞射,無測定出其他的化合物相之繞射峰值。又,相對密度為98.5%,比電阻值為105Ω・cm。將該等結果顯示於表1。(Example 9) In Example 9, the ratio of the atomic ratio of Sn and Zn Sn / (Sn + Zn) was 0.23, and the sintering holding temperature was set to 1400 ° C. In the same manner as in Example 1, a Sn-Zn-O-based oxide sintered body of Example 9 was obtained. As a result of X-ray diffraction analysis of the powder in the same manner as in Example 1, the Zn 2 SnO 4 phase of the spinel crystal structure was 74%, and the ZnO phase of the wurtzite crystal structure was 26% of the whole. The diffraction peaks of other compound phases were not measured. The relative density was 98.5%, and the specific resistance was 105Ω ・ cm. These results are shown in Table 1.

(實施例10)   於實施例10中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.3之比例進行調配,以使第1添加元素Ge之原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.0005、使第2添加元素Ta之原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.0005、及使第3添加元素Ga之原子數比Ga/(Sn+Zn+Ge+Ta+Ga)成為0.001的方式來調配GeO2 粉、Ta2 O5 粉、及Ga2 O3 粉,燒結保持時間為15小時,除此之外,以與實施例1相同方式,而得到實施例10之Sn-Zn-O系氧化物燒結體。與實施例6相同地,纖鋅礦型ZnO相為5%、及尖晶石型結晶構造之Zn2 SnO4 相為95%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為94.0%,比電阻值為12000Ω・cm。將該等結果顯示於表1。(Example 10) In Example 10, the ratio of the atomic ratio Sn / (Sn + Zn) of Sn and Zn to 0.3 was adjusted so that the atomic ratio of the first additive element Ge was Ge / (Sn + Zn). + Ge + Ta + Ga) is 0.0005, the atomic ratio of the second additive element Ta is Ta / (Sn + Zn + Ge + Ta + Ga) is 0.0005, and the atomic ratio of the third additive element Ga is Ga / ( Sn + Zn + Ge + Ta + Ga) was set to 0.001 to mix GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder, and the sintering retention time was 15 hours. In the same manner, the Sn-Zn-O-based oxide sintered body of Example 10 was obtained. As in Example 6, the wurtzite-type ZnO phase was 5%, and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 95% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 94.0%, and the specific resistance value was 12000 Ω ・ cm. These results are shown in Table 1.

(實施例11)   於實施例11中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.3之比例進行調配,以使第1添加元素Ge之原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.01、使第2添加元素Ta之原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.01、及使第3添加元素Ga之原子數比Ga/(Sn+Zn+Ge+Ta+Ga)成為0.1的方式來調配GeO2 粉、Ta2 O5 粉、及Ga2 O3 粉,燒結保持時間為25小時,除此之外,以與實施例1相同方式,而得到實施例11之Sn-Zn-O系氧化物燒結體。與實施例3相同地,纖鋅礦型ZnO相為5%、及尖晶石型結晶構造之Zn2 SnO4 相為95%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為95.5%,比電阻值為10500Ω・cm。將該等結果顯示於表1。(Example 11) In Example 11, the ratio of the atomic ratio Sn / (Sn + Zn) of Sn and Zn to 0.3 was adjusted so that the atomic ratio of the first additive element Ge was Ge / (Sn + Zn). + Ge + Ta + Ga) is 0.01, the atomic ratio of the second additive element Ta is Ta / (Sn + Zn + Ge + Ta + Ga) is 0.01, and the atomic ratio of the third additive element Ga is Ga / ( Sn + Zn + Ge + Ta + Ga) was adjusted to 0.1 so that GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder were prepared, and the sintering retention time was 25 hours. In the same manner, the Sn-Zn-O-based oxide sintered body of Example 11 was obtained. As in Example 3, the wurtzite-type ZnO phase was 5%, and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 95% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 95.5%, and the specific resistance value was 10,500 Ω ・ cm. These results are shown in Table 1.

(實施例12)   於實施例12中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.1之比例進行調配,以使第1添加元素Ge之原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.01、使第2添加元素Ta之原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.01、及使第3添加元素Ga之原子數比Ga/(Sn+Zn+Ge+Ta+Ga)成為0.1的方式來調配GeO2 粉、Ta2 O5 粉、及Ga2 O3 粉,將昇溫速度設為0.3℃/min,除此之外,以與實施例1相同方式,而得到實施例12之Sn-Zn-O系氧化物燒結體。與實施例2相同地,纖鋅礦型ZnO相為70%、及尖晶石型結晶構造之Zn2 SnO4 相為30%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為95.0%,比電阻值為1320Ω・cm。將該等結果顯示於表1。(Example 12) In Example 12, the ratio of the atomic ratio of Sn and Zn Sn / (Sn + Zn) was set to 0.1 so that the atomic ratio of the first additive element Ge was Ge / (Sn + Zn). + Ge + Ta + Ga) is 0.01, the atomic ratio of the second additive element Ta is Ta / (Sn + Zn + Ge + Ta + Ga) is 0.01, and the atomic ratio of the third additive element Ga is Ga / ( Sn + Zn + Ge + Ta + Ga) is set to 0.1 so that GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder are blended, and the heating rate is set to 0.3 ° C./min. In the same manner as in Example 1, a Sn-Zn-O-based oxide sintered body of Example 12 was obtained. As in Example 2, the wurtzite-type ZnO phase was 70%, and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 30% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 95.0%, and the specific resistance value was 1,320 Ω ・ cm. These results are shown in Table 1.

(實施例13)   於實施例13中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.1之比例進行調配,以使第1添加元素Ge之原子數比Ge/(Sn+Zn+Ge+Ta+Ga)成為0.0005、使第2添加元素Ta之原子數比Ta/(Sn+Zn+Ge+Ta+Ga)成為0.0005、及使第3添加元素Ga之原子數比Ga/(Sn+Zn+Ge+Ta+Ga)成為0.001的方式來調配GeO2 粉、Ta2 O5 粉、及Ga2 O3 粉,將昇溫速度設為1.0℃/min,除此之外,以與實施例1相同方式,而得到實施例13之Sn-Zn-O系氧化物燒結體。與實施例2相同地,纖鋅礦型ZnO相為70%、及尖晶石型結晶構造之Zn2 SnO4 相為30%繞射。無測定出其他的化合物相之繞射峰值。又,相對密度為94.5%,比電阻值為6800Ω・cm。將該等結果顯示於表1。(Example 13) In Example 13, the ratio of the atomic ratio Sn / (Sn + Zn) of Sn and Zn to 0.1 was adjusted so that the atomic ratio of the first additive element Ge was Ge / (Sn + Zn). + Ge + Ta + Ga) is 0.0005, the atomic ratio of the second additive element Ta is Ta / (Sn + Zn + Ge + Ta + Ga) is 0.0005, and the atomic ratio of the third additive element Ga is Ga / ( Sn + Zn + Ge + Ta + Ga) was adjusted to 0.001 to mix GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder, and the heating rate was set to 1.0 ° C./min. In the same manner as in Example 1, a Sn-Zn-O-based oxide sintered body of Example 13 was obtained. As in Example 2, the wurtzite-type ZnO phase was 70%, and the spinel-type crystal structure of the Zn 2 SnO 4 phase was 30% diffraction. No diffraction peak was measured for the other compound phases. The relative density was 94.5%, and the specific resistance was 6800 Ω ・ cm. These results are shown in Table 1.

(比較例1)   於比較例1中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.05之比例進行調配,除此之外,以與實施例1相同方式,而得到比較例1之Sn-Zn-O系氧化物燒結體。針對比較例1之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為90%、及尖晶石型結晶構造之Zn2 SnO4 相為10%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為93.0%,比電阻值為3510Ω・cm。亦即,確認無法達成相對密度為94%以上與比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 1) In Comparative Example 1, a comparative example was obtained in the same manner as in Example 1 except that the atomic ratio of Sn and Zn was Sn / (Sn + Zn) at a ratio of 0.05. Sn-Zn-O-based oxide sintered body of No. 1. For the Sn-Zn-O-based oxide sintered body of Comparative Example 1, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 90% and the spinel-type crystal structure was The Zn 2 SnO 4 phase is 10% diffraction. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance, the relative density was 93.0%, and the specific resistance was 3510 Ω ・ cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5 Ω ・ cm or more and 12000 Ω ・ cm or less could not be achieved. The results are shown in Table 2.

(比較例2)   於比較例2中,以Sn與Zn之原子數比Sn/(Sn+Zn)成為0.40之比例進行調配,除此之外,以與實施例1相同方式,而得到比較例2之Sn-Zn-O系氧化物燒結體。針對比較例2之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為0%、金紅石型SnO2 相為14%、及尖晶石型結晶構造之Zn2 SnO4 相為86%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為89.0%,比電阻值為597000Ω・cm。亦即,確認無法達成相對密度為94%以上且比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 2) In Comparative Example 2, a comparison example was obtained in the same manner as in Example 1 except that the atomic ratio Sn / (Sn + Zn) of Sn and Zn was adjusted to a ratio of 0.40. 2 of Sn-Zn-O based oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 2, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 0% and the rutile-type SnO 2 phase was 14 %, And the spinel-type crystal structure of the Zn 2 SnO 4 phase is 86% diffraction. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance value, the relative density was 89.0%, and the specific resistance value was 597,000 Ω ・ cm. That is, it was confirmed that it was impossible to achieve a relative density of 94% or more and a specific resistance of 5 Ω ・ cm or more and 12000 Ω 无法 cm or less. The results are shown in Table 2.

(比較例3)   於比較例3中,將昇溫速度設為0.2℃/min,除此之外,以與實施例1相同方式,而得到比較例3之Sn-Zn-O系氧化物燒結體。針對比較例3之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為90.0%,比電阻值為15000Ω・cm。亦即,確認無法達成相對密度為94%以上與比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 3) A Sn-Zn-O-based oxide sintered body of Comparative Example 3 was obtained in the same manner as in Example 1 except that the heating rate was set to 0.2 ° C / min in Comparative Example 3. . For the Sn-Zn-O-based oxide sintered body of Comparative Example 3, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure was The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance, the relative density was 90.0%, and the specific resistance was 15000 Ω ・ cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5 Ω ・ cm or more and 12000 Ω ・ cm or less could not be achieved. The results are shown in Table 2.

(比較例4)   於比較例4中,將昇溫速度設為1.2℃/min,除此之外,以與實施例1相同方式,而得到比較例4之Sn-Zn-O系氧化物燒結體。針對比較例4之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為92.0%,比電阻值為12500Ω・cm。亦即,確認無法達成相對密度為94%以上且比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 4) A Sn-Zn-O-based oxide sintered body of Comparative Example 4 was obtained in the same manner as in Example 1 except that the heating rate was set to 1.2 ° C / min in Comparative Example 4. . For the Sn-Zn-O-based oxide sintered body of Comparative Example 4, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure was the same. The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance, the relative density was 92.0%, and the specific resistance was 12500 Ω ・ cm. That is, it was confirmed that it was impossible to achieve a relative density of 94% or more and a specific resistance of 5 Ω ・ cm or more and 12000 Ω 无法 cm or less. The results are shown in Table 2.

(比較例5)   於比較例5中,將燒結溫度設為1280℃,除此之外,以與實施例1相同方式,而得到比較例5之Sn-Zn-O系氧化物燒結體。針對比較例5之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為91.0%,比電阻值為14000Ω・cm。亦即,確認無法達成相對密度為94%以上且比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 5) A Sn-Zn-O-based oxide sintered body of Comparative Example 5 was obtained in the same manner as in Example 1 except that the sintering temperature was set to 1280 ° C. For the Sn-Zn-O-based oxide sintered body of Comparative Example 5, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure was the same. The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance, the relative density was 91.0%, and the specific resistance was 14000 Ω ・ cm. That is, it was confirmed that it was impossible to achieve a relative density of 94% or more and a specific resistance of 5 Ω ・ cm or more and 12000 Ω 无法 cm or less. The results are shown in Table 2.

(比較例6)   於比較例6中,將燒結溫度設為1430℃,除此之外,以與實施例1相同方式,而得到比較例6之Sn-Zn-O系氧化物燒結體。針對比較例6之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為93.0%,比電阻值為12500Ω・cm。亦即,確認無法達成相對密度為94%以上且比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 6) A Sn-Zn-O-based oxide sintered body of Comparative Example 6 was obtained in the same manner as in Example 1 except that the sintering temperature was set to 1,430 ° C in Comparative Example 6. For the Sn-Zn-O-based oxide sintered body of Comparative Example 6, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure was The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance, the relative density was 93.0%, and the specific resistance was 12500 Ω ・ cm. That is, it was confirmed that it was impossible to achieve a relative density of 94% or more and a specific resistance of 5 Ω ・ cm or more and 12000 Ω 无法 cm or less. The results are shown in Table 2.

(比較例7)   於比較例7中,將以1350℃之燒結的保持時間設為10小時,除此之外,以與實施例1相同方式,而得到比較例7之Sn-Zn-O系氧化物燒結體。針對比較例7之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為90.0%,比電阻值為13500Ω・cm。亦即,確認無法達成相對密度為94%以上且比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 7) In Comparative Example 7, a Sn-Zn-O system of Comparative Example 7 was obtained in the same manner as in Example 1 except that the holding time of sintering at 1350 ° C was set to 10 hours. An oxide sintered body. The Sn-Zn-O-based oxide sintered body of Comparative Example 7 was subjected to X-ray diffraction analysis in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure was the same. The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance value, the relative density was 90.0%, and the specific resistance value was 13,500 Ω ・ cm. That is, it was confirmed that it was impossible to achieve a relative density of 94% or more and a specific resistance of 5 Ω ・ cm or more and 12000 Ω 无法 cm or less. The results are shown in Table 2.

(比較例8)   於比較例8中,將以1350℃之燒結的保持時間設為30小時,除此之外,以與實施例1相同方式,而得到比較例8之Sn-Zn-O系氧化物燒結體。針對比較例8之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,有ZnO或Zn2 SnO4 之揮發,而相對密度為93.0%,比電阻值為13000Ω・cm。亦即,確認無法達成相對密度為94%以上且比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 8) In Comparative Example 8, the Sn-Zn-O system of Comparative Example 8 was obtained in the same manner as in Example 1 except that the holding time of sintering at 1350 ° C was set to 30 hours. An oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 8, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure was the same. The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. In addition, as a result of measuring the relative density and specific resistance value, there was volatilization of ZnO or Zn 2 SnO 4 , the relative density was 93.0%, and the specific resistance value was 13000 Ω ・ cm. That is, it was confirmed that it was impossible to achieve a relative density of 94% or more and a specific resistance of 5 Ω ・ cm or more and 12000 Ω 无法 cm or less. The results are shown in Table 2.

(比較例9)   於比較例9中,以Ge/(Sn+Zn+Ge+Ta+Ga)成為0.03之比例進行調配,除此之外,以與實施例1相同方式,而得到比較例9之Sn-Zn-O系氧化物燒結體。針對比較例9之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為93.0%,比電阻值為8500Ω・cm。亦即,確認無法達成相對密度為94%以上。將結果顯示於表2。(Comparative Example 9) Comparative Example 9 was prepared in the same manner as in Example 1 except that Ge / (Sn + Zn + Ge + Ta + Ga) was adjusted to a ratio of 0.03, and Comparative Example 9 was obtained. Sn-Zn-O based oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 9, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure was the same. The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance, the relative density was 93.0%, and the specific resistance was 8500 Ω ・ cm. That is, it was confirmed that the relative density could not be achieved at 94% or more. The results are shown in Table 2.

(比較例10)   於比較例10中,以Ge/(Sn+Zn+Ge+Ta+Ga)成為0.0001之比例進行調配,除此之外,以與實施例1相同方式,而得到比較例10之Sn-Zn-O系氧化物燒結體。針對比較例10之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為91.0%,比電阻值為9800Ω・cm。亦即,確認無法達成相對密度為94%以上。將結果顯示於表2。(Comparative Example 10) Comparative Example 10 was prepared in the same manner as in Example 1 except that Ge / (Sn + Zn + Ge + Ta + Ga) became 0.0001, and Comparative Example 10 was obtained. Sn-Zn-O based oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 10, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance, the relative density was 91.0%, and the specific resistance was 9800 Ω ・ cm. That is, it was confirmed that the relative density could not be achieved at 94% or more. The results are shown in Table 2.

(比較例11)   於比較例11中,以Ta/(Sn+Zn+Ge+Ta+Ga)成為0.03之比例進行調配,除此之外,以與實施例1相同方式,而得到比較例11之Sn-Zn-O系氧化物燒結體。針對比較例11之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為97.0%,比電阻值為16000Ω・cm。亦即,確認無法達成比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 11) Comparative Example 11 was prepared in the same manner as in Example 1 except that Ta / (Sn + Zn + Ge + Ta + Ga) was adjusted to a ratio of 0.03, and Comparative Example 11 was obtained. Sn-Zn-O based oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 11, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance value, the relative density was 97.0%, and the specific resistance value was 16000 Ω ・ cm. That is, it was confirmed that the specific resistance could not be higher than 5 Ω ・ cm and lower than 12000 Ω ・ cm. The results are shown in Table 2.

(比較例12)   於比較例12中,以Ta/(Sn+Zn+Ge+Ta+Ga)成為0.0001之比例進行調配,除此之外,以與實施例1相同方式,而得到比較例12之Sn-Zn-O系氧化物燒結體。針對比較例12之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為96.7%,比電阻值為25000Ω・cm。亦即,確認無法達成比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 12) Comparative Example 12 was prepared in the same manner as in Example 1 except that Ta / (Sn + Zn + Ge + Ta + Ga) was set to a ratio of 0.0001, and Comparative Example 12 was obtained. Sn-Zn-O based oxide sintered body. The Sn-Zn-O-based oxide sintered body of Comparative Example 12 was subjected to X-ray diffraction analysis in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel-type crystal structure was The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance value, the relative density was 96.7%, and the specific resistance value was 25000 Ω ・ cm. That is, it was confirmed that the specific resistance could not be higher than 5 Ω ・ cm and lower than 12000 Ω ・ cm. The results are shown in Table 2.

(比較例13)   於比較例13中,以Ga/(Sn+Zn+Ge+Ta+Ga)成為0.2之比例進行調配,除此之外,以與實施例1相同方式,而得到比較例13之Sn-Zn-O系氧化物燒結體。針對比較例13之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為97.3%,比電阻值為14800Ω・cm。亦即,確認無法達成比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 13) Comparative Example 13 was obtained in the same manner as in Example 1 except that Ga / (Sn + Zn + Ge + Ta + Ga) was set to a ratio of 0.2, and Comparative Example 13 was obtained. Sn-Zn-O based oxide sintered body. The Sn-Zn-O-based oxide sintered body of Comparative Example 13 was subjected to X-ray diffraction analysis in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel crystal structure The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance, the relative density was 97.3%, and the specific resistance was 14800 Ω ・ cm. That is, it was confirmed that the specific resistance could not be higher than 5 Ω ・ cm and lower than 12000 Ω ・ cm. The results are shown in Table 2.

(比較例14)   於比較例14中,以Ga/(Sn+Zn+Ge+Ta+Ga)成為0.0008之比例進行調配,除此之外,以與實施例1相同方式,而得到比較例14之Sn-Zn-O系氧化物燒結體。針對比較例14之Sn-Zn-O系氧化物燒結體,與實施例1相同地,進行X射線繞射分析之結果,纖鋅礦型ZnO相為34%、及尖晶石型結晶構造之Zn2 SnO4 相為66%繞射。無測定出其他的化合物相之繞射峰值。又,測定相對密度與比電阻值之結果,相對密度為97.0%,比電阻值為22000Ω・cm。亦即,確認無法達成比電阻5Ω・cm以上12000Ω・cm以下。將結果顯示於表2。(Comparative Example 14) Comparative Example 14 was prepared in the same manner as in Example 1 except that Ga / (Sn + Zn + Ge + Ta + Ga) was set to a ratio of 0.0008, and Comparative Example 14 was obtained. Sn-Zn-O based oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 14, the results of X-ray diffraction analysis were performed in the same manner as in Example 1. The wurtzite-type ZnO phase was 34% and the spinel crystal structure The Zn 2 SnO 4 phase is 66% diffracted. No diffraction peak was measured for the other compound phases. As a result of measuring the relative density and specific resistance value, the relative density was 97.0%, and the specific resistance value was 22000 Ω ・ cm. That is, it was confirmed that the specific resistance could not be higher than 5 Ω ・ cm and lower than 12000 Ω ・ cm. The results are shown in Table 2.

另外,如上述般地針對本發明之一實施形態及各實施例詳細地進行了說明,但,可不實際脫離本發明之新穎事項及效果的多種變形一事係該業者可容易理解。因而,如此之變形例全部包含於本發明之範圍內。In addition, as described above, one embodiment of the present invention and each embodiment have been described in detail, but those skilled in the art can easily understand that various modifications can be made without actually departing from the novel matters and effects of the present invention. Therefore, all such modifications are included in the scope of the present invention.

例如,於說明書或圖式中,至少一次被與更廣義或同義之不同的用語一同記載的用語係於說明書或圖式之任何地方皆可替換成其之不同的用語。又,Sn-Zn-O系氧化物燒結體與其製造方法的構成亦不限定於本發明之一實施形態及各實施例所說明者,可實施各種的變形。For example, in a description or a drawing, a term that is described at least once with a different term that is more broadly or synonymously is replaced with a different term anywhere in the description or the drawing. The structure of the Sn-Zn-O-based oxide sintered body and the method for producing the same are not limited to those described in one embodiment of the present invention and the examples, and various modifications can be made.

[第1圖]第1圖係顯示本發明之一實施形態之Sn-Zn-O系氧化物燒結體的製造方法之製程的概略之步驟圖。[Fig. 1] Fig. 1 is a schematic diagram showing a process of a method for producing a Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention.

Claims (6)

一種Sn-Zn-O系氧化物燒結體,其係具有鋅(Zn)與錫(Sn)作為成分之Sn-Zn-O系氧化物燒結體,其特徵為,   進一步含有至少鍺(Ge)、鉭(Ta)、及鎵(Ga)作為成分,   金屬原子數比係   Sn/(Zn+Sn)為0.1以上0.3以下、   Ge/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、   Ta/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、   Ga/(Zn+Sn+Ge+Ta+Ga)為0.001以上0.1以下,   比電阻為5Ω・cm以上12000Ω・cm以下,相對密度為94%以上。A Sn-Zn-O-based oxide sintered body, which is a Sn-Zn-O-based oxide sintered body having zinc (Zn) and tin (Sn) as components, wherein ytterbium further contains at least germanium (Ge), Tantalum (Ta) and gallium (Ga) as components, the ratio of rhenium metal atomic ratio Sn / (Zn + Sn) is 0.1 or more and 0.3 or less, Ge / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less, Ta / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less, Ga / (Zn + Sn + Ge + Ta + Ga) is 0.001 or more and 0.1 or less, and specific resistance is 5Ω ・ cm or more and 12000Ω ・ cm or less. The relative density is above 94%. 如請求項1之Sn-Zn-O系氧化物燒結體,其中,前述金屬原子數比係Sn/(Zn+Sn)為0.16以上0.23以下,   前述比電阻為5Ω・cm以上110Ω・cm以下,前述相對密度為98%以上。For example, the sintered body of Sn-Zn-O oxide according to claim 1, wherein the metal atomic ratio Sn / (Zn + Sn) is 0.16 or more and 0.23 or less, and the specific resistance is 5Ω ・ cm or more and 110Ω ・ cm or less, The aforementioned relative density is 98% or more. 如請求項1之Sn-Zn-O系氧化物燒結體,其中,   以纖鋅礦型結晶構造之ZnO相為全體的5~70%之範圍,或尖晶石型結晶構造之Zn2 SnO4 相為全體的30~95%之範圍所構成。For example, the Sn-Zn-O-based oxide sintered body according to claim 1, wherein the ZnO phase having a wurtzite type crystal structure is in a range of 5 to 70% of the whole, or Zn 2 SnO 4 having a spinel type crystal structure. The phase is constituted by a range of 30 to 95% of the whole. 如請求項2之Sn-Zn-O系氧化物燒結體,其中,   以纖鋅礦型結晶構造之ZnO相為全體的5~70%之範圍,或尖晶石型結晶構造之Zn2 SnO4 相為全體的30~95%之範圍所構成。For example, the Sn-Zn-O-based oxide sintered body according to claim 2, wherein the ZnO phase with a wurtzite-type crystal structure is in a range of 5 to 70% of the whole, or Zn 2 SnO 4 with a spinel-type crystal structure. The phase is constituted by a range of 30 to 95% of the whole. 一種Sn-Zn-O系氧化物燒結體之製造方法,其係具有鋅(Zn)與錫(Sn)作為成分之Sn-Zn-O系氧化物燒結體之製造方法,其特徵為具有下列步驟:   將鋅之氧化物粉末、錫之氧化物粉末、及含有添加元素之氧化物粉末進行混合,而製作造粒粉末的造粒步驟;   將前述造粒粉末進行加壓成形,而得到成形體的成形步驟;以及   將前述成形體進行燒成,而得到氧化物燒結體的燒成步驟,   前述添加元素係至少鍺(Ge)、鉭(Ta)、及鎵(Ga),   以使金屬原子數比成為   Sn/(Zn+Sn)為0.1以上0.3以下、   Ge/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、   Ta/(Zn+Sn+Ge+Ta+Ga)為0.0005以上0.01以下、   Ga/(Zn+Sn+Ge+Ta+Ga)為0.001以上0.1以下   的方式來將前述鋅之氧化物粉末、前述錫之氧化物粉末、及前述含有添加元素之氧化物粉末進行混合。A method for manufacturing a Sn-Zn-O-based oxide sintered body, which is a method for manufacturing a Sn-Zn-O-based oxide sintered body having zinc (Zn) and tin (Sn) as components, which is characterized by having the following steps : A granulation step of preparing a granulated powder by mixing zinc oxide powder, tin oxide powder, and an oxide powder containing an additive element; press-forming the granulated powder to obtain a molded body A forming step; and a firing step of firing the formed body to obtain an oxide sintered body, the aforementioned additive element is at least germanium (Ge), tantalum (Ta), and gallium (Ga), and so that the metal atomic ratio is Sn / (Zn + Sn) is 0.1 or more and 0.3 or less, Ge / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 or less, Ta / (Zn + Sn + Ge + Ta + Ga) is 0.0005 or more and 0.01 Hereinafter, the zinc oxide powder, the tin oxide powder, and the additive element-containing oxide powder are mixed so that Ga / (Zn + Sn + Ge + Ta + Ga) is 0.001 or more and 0.1 or less. 如請求項5之Sn-Zn-O系氧化物燒結體之製造方法,其中,於前述燒成步驟中係在大氣中之燒成爐內環境下,以昇溫速度為0.3~1.0℃/min昇溫至1300℃以上1400℃以下、15小時以上25小時以內之條件,來將前述成形體進行燒成。For example, the method for producing a Sn-Zn-O-based oxide sintered body according to claim 5, wherein the temperature in the firing furnace is in the atmosphere of a firing furnace in the aforementioned firing step, and the temperature is raised at a rate of 0.3 to 1.0 ° C / min. The molded body is fired to a temperature of 1300 ° C or higher and 1400 ° C or lower and within 15 hours to 25 hours.
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