TWI741154B - Sn-Zn-O series oxide sintered body and its manufacturing method - Google Patents
Sn-Zn-O series oxide sintered body and its manufacturing method Download PDFInfo
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Abstract
本發明係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。本發明之Sn-Zn-O系氧化物燒結體係具有鋅(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。The present invention provides a high-density and low-resistance Sn-Zn-O-based oxide sintered body that can be used in applications such as barrier films or protective films, and a method for manufacturing the same. The Sn-Zn-O-based oxide sintered system of the present invention has zinc (Zn) and tin (Sn) as the components of the Sn-Zn-O-based oxide sintered body, which further contains at least germanium (Ge), tantalum (Ta ), and gallium (Ga) as components, and the metal atom number 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 to 0.01, Ga/(Zn+Sn+Ge+Ta+Ga) is 0.001 to 0.1, specific resistance is 5Ω・cm to 12000Ω・cm, relative density It is more than 94%.
Description
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 present invention relates to Sn-Zn used as a sputtering target when a transparent conductive film suitable for solar cells, liquid crystal surface elements, touch panels, etc. is manufactured by the sputtering method of DC sputtering and high-frequency sputtering -O-based oxide sintered body and its manufacturing method. This application is based on the Japanese patent application number Japanese Patent Application No. 2017-095982 filed in Japan on May 12, 2017, and claims priority, and the content of the application is incorporated into this application 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 with high conductivity and high transmittance in the visible light region are used in solar cells, liquid crystal display devices, organic electroluminescence, inorganic electroluminescence, and other surface elements, or touch panel electrodes, 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 for automobile windows or construction.
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 containing tin as a dopant ( In 2 O 3 ) and so on. In particular, an indium oxide (In 2 O 3 ) film containing tin as a dopant, that is, an In-Sn-O film system is called an ITO (Indium tin oxide) film, because it is easy to obtain a low-resistance film , 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 the manufacturing method of the above-mentioned transparent conductive film, the sputtering method of direct current sputtering and high frequency sputtering is often used. When it is necessary to form a film of a material with a low vapor pressure or to control a precise film thickness, the sputtering method is an effective method. 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 above-mentioned transparent conductive film, conventionally, indium oxide-based materials such as ITO have been widely used. However, indium metal is a rare metal on the earth and is toxic. Therefore, there is a concern about adverse effects on the environment or the human body, and non-indium-based materials are required.
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 aforementioned non-indium-based materials, as described above, zinc oxide (ZnO)-based materials containing aluminum or gallium as a dopant, and tin oxide (SnO 2 )-based materials 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 the sputtering method, but it has disadvantages such as lack of chemical resistance (alkali resistance and acid resistance). On the other hand, although the transparent conductive film of tin oxide (SnO 2 )-based materials is excellent in chemical resistance, it is difficult to produce high-density and durable tin oxide-based sintered target materials. Therefore, it is difficult to use sputtering. Method to manufacture the above-mentioned shortcomings of the 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 to improve these shortcomings, a sintered body containing 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 crystal phase of tin oxide or a crystal phase of tin oxide in which zinc is dissolved, but a zinc oxide phase and tin oxide phase It is composed of zinc acid compound phase or 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, in Patent Document 2 describes a sintered body based average grain size of 4.5μm or less, and when using CuKα rays have an X-ray diffraction of Zn (222) 2 SnO 4 phase plane, ( When the cumulative intensity of 400) surface is set to I (222) and I (400) , the orientation degree expressed by I (222) /[I (222) +I (400) ] is greater than the standard (0.44) 0.52 or more. Furthermore, Patent Document 2 also describes as a method of manufacturing a sintered body having the above-mentioned characteristics, a method of constructing a manufacturing step of the sintered body by the following steps: In the environment, the step of sintering the molded body under the condition of 800℃~1400℃; and after the holding at the highest sintering temperature, the inside of the sintering furnace is cooled by an inert environment such as Ar gas step. [Prior Technical Documents] [Patent Documents]
[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 Application Publication No. 2007-277075 [Patent Document 2] Japanese Patent Application Publication No. 2013-036073
[發明所欲解決之課題][The problem 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, in the Sn-Zn-O-based oxide sintered body with Zn and Sn as the main components, although the strength of the sintered body that can withstand mechanical strength can be obtained, it is difficult to obtain sufficient density or electrical conductivity. As a characteristic required for sputtering film formation at the mass production site, it cannot be satisfied. That is, in the normal pressure sintering method, there are still problems in achieving high density or electrical 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 series oxide sintered body with Zn and Sn as the main components is made of materials that are difficult to have the characteristics of high density and low resistance. Even if the blending ratio of Sn and Zn is changed, it is difficult to produce high density and An oxide sintered body with excellent conductivity. In the density of the sintered body, although there is a slight fluctuation in the density due to the blending ratio, the conductivity shows a very high specific resistance value of 1×10 6 Ω・cm or more, and the conductivity is lacking.
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 body with Zn and Sn as the main components, Zn 2 SnO 4 compounds are formed from around 1100°C, and Zn volatilization starts at around 1400°C, starting at around 1450°C The volatilization of Zn becomes obvious. If the Sn-Zn-O-based oxide sintered body is fired at a high temperature in order to increase the density, the volatilization of Zn progresses, so the grain boundary diffusion or the bond between the 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。In addition, regarding conductivity, Zn 2 SnO 4 , ZnO, and SnO 2 are poor in conductivity. Therefore, even if the blending ratio is adjusted to adjust the compound phase or the amount of ZnO and SnO 2 , the conductivity cannot be greatly 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. By sputtering the sintered body as a target, it is suitable for use as a transparent conductive film for liquid crystals, solar cells, etc. . On the other hand, in recent years, there have been applications in which the conductivity is worse than ITO, but can be used for gas barrier films, water vapor barrier films, and other barrier films or protective films for protection 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, the subject of the present invention is to provide a high-density and low-resistance Sn-Zn-O-based oxide sintered body that can be used in applications such as barrier films or protective films, and a method of manufacturing 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 inventors of the present invention have found that in order to solve the above-mentioned problems, Sn is contained in a ratio of Sn/(Sn+Zn) of 0.1 or more and 0.3 or less as the atomic ratio, and Ge, Ta, and Ga are contained in a specific ratio as an additive element. There are three types, and a high-density Sn-Zn-O oxide sintered body with a specific resistance value of about 10Ω・cm~×10 4 Ω・cm suitable for barrier films or protective films can be obtained, thus completing this 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 same state of the present invention is a Sn-Zn-O-based oxide sintered body having zinc (Zn) and tin (Sn) as components, which further contains at least germanium (Ge), tantalum (Ta), and gallium (Ga) as a component, and the metal atom number ratio is Sn/(Zn+Sn) 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, specific resistance is 5Ω・cm or more and 12000Ω・cm or less, 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 same aspect of the present invention, by making Sn/(Sn+Zn) a ratio of 0.1 or more and 0.3 or less, and using three kinds of germanium (Ge), tantalum (Ta), and gallium (Ga) as additional elements, Instead, it can be used as a high-density and low-resistance Sn-Zn-O-based oxide sintered body that can be used in applications such as barrier films and protective films.
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 same state of the present invention, the metal atom number ratio Sn/(Zn+Sn) can be set to be 0.16 or more and 0.23 or less, the specific resistance should be 5Ω・cm or more and 110Ω・cm or less, and the relative density can be 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。In this way, by further limiting Sn/(Zn+Sn), a Sn-Zn-O-based oxide sintered body with high density and 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 addition, in the same aspect of the present invention, in the Sn-Zn-O-based oxide sintered body, the ZnO phase that can be set as a wurtzite-type crystal structure is 5 to 70% of the total (in this specification, "~ It is set to mean the range above the lower limit and below the upper limit, the same below), or the Zn 2 SnO 4 phase of the spinel crystal structure is constituted in the 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 composed of 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。In addition, another aspect of the present invention is a method for manufacturing a Sn-Zn-O-based oxide sintered body having zinc (Zn) and tin (Sn) as components, which includes the following steps: A granulation process of mixing the oxide powder and the oxide powder containing the added element to produce a granulated powder; a molding step of press-forming the granulated powder to obtain a molded body; and firing the molded body In the firing step to obtain the oxide sintered body, the aforementioned additional elements are at least germanium (Ge), tantalum (Ta), and gallium (Ga), so that the ratio of metal atoms is Sn/(Zn+Sn) of 0.1 or more and 0.3 Below, Ge/(Zn+Sn+Ge+Ta+Ga) is above 0.0005 and below 0.01, Ta/(Zn+Sn+Ge+Ta+Ga) is above 0.0005 and below 0.01, 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 oxide powder containing the additive element.
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 kinds of germanium (Ge), tantalum (Ta), and gallium (Ga) are used as an additive element by making Sn/(Zn+Sn) a ratio of 0.1 to 0.3. By mixing in a specific ratio, it is possible to produce a high-density and low-resistance Sn-Zn-O-based oxide sintered body that can be used in applications such as barrier films or 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 to raise the temperature in the firing step in the atmosphere of the firing furnace at a rate of temperature rise of 0.3-1.0°C/min to 1300°C or more and 1400°C or less , 15 hours to 25 hours, to sinter the aforementioned molded body.
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 manufactured. [Effects of the invention]
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, a high-density and low-resistance Sn-Zn-O-based oxide sintered body can be used for applications such as barrier films or protective films.
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 of the present invention and its manufacturing method will be described in the following order with reference to the drawings. In addition, 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. Manufacturing method of Sn-Zn-O-based oxide sintered body 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 sintered system of one embodiment of the present invention contains Sn as an atomic ratio Sn/(Sn+Zn) of 0.1 to 0.3 in proportion to the total amount of all metal elements. The atomic number ratio Ge/(Sn+Zn+Ge+Ta+ Ga) is 0.0005 or more and 0.01 or less, and the first additional element Ge is included, and the atomic number ratio Ta/(Sn+Zn +Ge +Ta+Ga) is 0.0005 or more and 0.01 or less, containing the second additional element Ta, and the atomic ratio Ga/(Sn+Zn+Ge+Ta+Ga) relative to the total amount of all metal elements is The third additive element Ga is contained in a ratio of 0.001 or more and 0.1 or less. In this way, the Sn-Zn-O-based oxide sintered system of one embodiment of the present invention has a specific resistance of 5Ω・cm or more and 12000Ω・cm or less, and a relative density of 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。The tin oxide and zinc oxide as the main raw materials of the Sn-Zn-O based oxide sintered body of one embodiment of the present invention will only be zinc oxide tin compounds, or raw material powders containing mixed powders of tin oxide and zinc oxide , Sn is contained in a ratio of Sn/(Sn+Zn) of 0.1 to 0.3 as the atomic ratio.
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 is observed in the crystal structure of the sintered body after sintering. When Sn is contained in a ratio of Sn/(Sn+Zn) of 0.1 to 0.3 as the atomic ratio, the ZnO phase of the wurtzite crystal structure and the Zn 2 SnO 4 phase of the spinel crystal structure are 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. If the main component of the SnO 2 phase of the rutile crystal structure increases, the resistance value increases. In addition, the transmittance will also 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 or more and 0.23 or less. If it is in this range, it will become a desired resistance value, and it will become 98% or more with respect to density, and it 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。In the production of Sn-Zn-O-based oxide sintered bodies, as mentioned above, during sintering, Zn 2 SnO 4 compounds start to be generated from around 1100°C, volatilization of Zn starts after 1400°C, and Zn starts at around 1450°C. The volatilization becomes obvious. If the Sn-Zn-O-based oxide sintered body is fired at a high temperature in order to increase the density, the volatilization of Zn progresses, so the grain boundary diffusion or the bond between the grains is weak, and high-density oxide sintering cannot be obtained. body. On the other hand, with regard to conductivity, Zn 2 SnO 4 , ZnO, and SnO 2 are materials that lack conductivity. Therefore, even if the blending ratio is adjusted to adjust the compound phase or the amount of ZnO and SnO 2 , the conductivity cannot be greatly improved. 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。(Additional element) ”Therefore, in the present invention, the first to third additional elements are added in order to improve the above-mentioned conductivity. That is, by adding germanium (Ge) as the first additional element, tantalum (Ta) as the second additional element, and gallium (Ga) as the third additional element, it becomes possible to obtain Sn-Zn with high density and low resistance. -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 additional element] In order to densify the oxide sintered body, the addition of Ge as the first additional element has the effect of obtaining a higher density. The first additive element Ge promotes the diffusion of grain boundaries and helps the growth of crystal necks between grains, so that the bonds between grains become strong and contribute to densification. Here, the reason why the atomic ratio Ge/(Sn+Zn+Ge+Ta+Ga) of the first additive element Ge to the total amount of all metal elements is set to 0.0005 or more and 0.01 or less is that the above-mentioned atomic number ratio Ge When / (Sn+Zn+Ge+Ta+Ga) is less than 0.0005, the effect of increasing the density cannot be exhibited (see Comparative Example 10). When the atomic ratio Ge/(Sn+Zn+Ge+Ta+Ga) exceeds 0.01, the effect of increasing the density cannot be exhibited (see Comparative Example 9). And it will generate other compounds, such as Zn 2 Ge 3 O 8 compounds.
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 Ge as the first additive element 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] Sn-Zn-O-based oxide sintered with the above-mentioned first additive element Ge under the condition that Sn is contained in a ratio of Sn/(Sn+Zn) of 0.1 to 0.3 as the atomic ratio Although the density of the system is increased as described above, there is still a problem in 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 additional element Ta is added. With the addition of the second additional element Ta, the conductivity is improved while maintaining the high density of the oxide sintered body. In addition, the second additional element Ta is an element with a valence of 5 or higher.
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 additional element Ta to the total amount of all metal elements 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 above-mentioned atomic ratio Ta/(Sn+Zn+Ge+Ta+Ga) exceeds 0.01, other compound phases such as Ta 2 O 5 , ZnTa 2 O 6 and the like will be formed. , Therefore, the conductivity deteriorates (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 additional element] As described above, the conductivity is improved by the addition of the second additional element Ta. However, Ta will replace with Sn and SnO 2 in the Zn 2 SnO 4 phase to be solid-soluted. Therefore, the conductivity of the desired resistance value 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 additional element Ga is added. The addition of the third additive element Ga is expected to improve the conductivity of Zn in 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 additional element Ge to the total amount of all metal elements is 0.001 or more and 0.1 or less. In the case where 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 Ga 2 O 3, etc. will be formed, which will lead to electrical conductivity. Sexual deterioration (refer to 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 it does not impair the characteristics of the Sn-Zn-O-based oxide sintered body as one of the embodiments of the present invention, it can be used in applications such as barrier films or protective films, with high density (relative density of 94% or more) and Those with a low resistance (specific resistance of 5Ω・cm or more and 12000Ω・cm or less) may further contain additional elements. 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 oxide sintered body of one embodiment of the present invention, when the atomic ratio Sn/(Sn+Zn) is 0.1 or more and 0.3 or less, the wurtzite type crystal The ZnO phase of the structure and the Zn 2 SnO 4 phase of the spinel crystal structure are the main components. In addition, the appropriate amount of the first additive element Ge, the second additive element Ta, and the third additive element Ga will be combined with the Zn in the ZnO phase. , Zn in the Zn 2 SnO 4 phase or Sn in the SnO 2 phase is replaced by Sn in the SnO 2 phase for solid solution. Therefore, the ZnO phase of the wurtzite crystal structure and the Zn 2 SnO 4 phase of the spinel crystal structure are other than Other compound phases will not be formed.
(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。(Resistivity) The specific resistance of the Sn-Zn-O-based oxide sintered body according to one 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 Sn-Zn-O oxide sintered body has conventionally been a very high specific resistance value of 1×10 6 Ω・cm or more. In the present invention, the specific resistance value is lowered by blending Ge, Ta, and Ga as the first to third additional 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 2~3×10 -4 Ω・cm. By sputtering this sintered body as a target, it is suitable for use as a transparent conductive film for liquid crystal or solar electronics. . The specific resistance of the transparent conductive film obtained by sputtering the Sn-Zn-O based oxide sintered body of one embodiment of the present invention is about 10Ω・cm to 1×10 4 Ω・cm. Therefore, the conductivity is It is inferior to ITO, but it can be used for gas barrier films, water vapor barrier films and other barrier films or protective films for protection from damage or impact. The Sn-Zn-O oxide sintered system of one embodiment of the present invention is suitable for sputtering specific resistance of films with a specific resistance of about 10Ω・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 forming conditions during the sputtering, especially the oxygen concentration during the sputtering. However, if considering the productivity during sputtering, the uniformity of the film, etc., it is better 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。In addition, the specific resistance value depends on the film formation speed during sputtering. Therefore, the smaller the specific resistance value, the better. The Sn-Zn-O-based oxide sintered body according to one embodiment of the present invention has a specific resistance of 5Ω・cm or more and 12000Ω・cm or less, and therefore becomes an oxide sintered body suitable for sputtering. In the case where the specific resistance is less than 5Ω・cm, the resistance value of the resulting film will become low, so leakage from nearby electrodes becomes a problem. In addition, if the specific resistance value exceeds 12000 Ω·cm, it becomes difficult to discharge, and the film cannot be formed stably with respect to DC sputtering, which becomes 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 making the ratio of the number of metal atoms of Sn/(Zn+Sn) 0.16 or more and 0.23 or less, the specific resistance value can be set in the range of 5Ω・cm or more and 110Ω・cm or less. (Refer to Examples 1, 8, 9). It is better to increase the film forming speed by making the specific resistance value 5Ω・cm or more and 110Ω・cm or less.
(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 one embodiment of the present invention is 94% or more. As shown in Patent Document 1, in the Sn-Zn-O oxide sintered body blended at an atomic ratio Sn/(Sn+Zn) of 0.23 or more and 0.5 or less, the relative density is due to the sintering At this time, Zn volatilizes and crystals with high relative density cannot be obtained. In the present invention, the relative density can be increased by blending the above-mentioned 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。In addition, by making the metal atom number ratio Sn/(Zn+Sn) 0.16 or more and 0.23 or less, the aforementioned relative density can be increased to 98% or more. When the relative density is 98% or more, the strength of the target material increases and the film formation speed during sputtering increases. At the same time, the outgassing due to the target material decreases, resulting in 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 manufacturing a Sn-Zn-O-based oxide sintered body having zinc (Zn) and tin (Sn) as components, which includes the following steps: oxidizing zinc oxide powder and tin The granulation step S1 of mixing the powder and the oxide powder containing the additive element to produce a granulated powder; the molding step S2 of press-forming the granulated powder to obtain a molded body; and firing the molded body Then, the firing step S3 of the oxide sintered body is obtained. For example, the Sn-Zn-O-based oxide sintering system of one embodiment of the present invention is a raw material powder containing only a zinc tin oxide compound or a mixed powder of tin oxide and zinc oxide, and the second is blended at a specific ratio 1. The germanium oxide of the additional element, the tantalum oxide of the second additional element, and the gallium oxide of the third additional element are granulated, and the granulated powder is formed by cold equalizing pressure, etc., and the formed body is fired in a sintering 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 the granulation step S1, the main raw material is prepared. The main raw materials of tin oxide and zinc oxide are only zinc oxide tin compounds, or raw material powders containing mixed powder of tin oxide and zinc oxide, as the atomic ratio Sn/ (Sn+Zn) is 0.1 or more and 0.3 or less The ratio contains Sn. If the main raw material is mixed powder of tin oxide and zinc oxide, it is easier to adjust the blending ratio, which is better. For example, the raw material powder is SnO 2 powder and ZnO powder. In addition, an oxide containing the first additional element to the third additional element is prepared, and is added to this main raw material for blending. For example, GeO 2 powder as the first additive element Ge , Ta 2 O 5 powder as the second additive element Ta, and 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 atom number ratio is 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 to combine zinc oxide powder, tin oxide powder, and The oxide powders containing added elements are mixed. In this way, so that the ratio of Sn/(Zn+Sn) is 0.1 or more and 0.3 or less, and as described above, three kinds of germanium (Ge), tantalum (Ta), and gallium (Ga) are specified as additional elements. By mixing in a proportion, it is possible to produce a high-density and low-resistance Sn-Zn-O-based oxide sintered body that can be used in applications such as barrier films and protective films.
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, pure water or ultrapure water, organic binder, dispersant, and defoamer are mixed in a mixing tank so that the concentration of the raw material powder becomes a specific concentration. In addition, using a bead mill or the like in which hard ZrO 2 balls are introduced, the raw material powder is wet-pulverized, and then mixed and stirred to obtain a slurry. By spraying and drying the obtained slurry with a spray drying device or the like, granulated powder can be obtained.
(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. Forming step) The forming step S2 is a step of press-forming the granulated powder obtained in the granulating step S1 to obtain a molded body. In the forming step S2, in order to remove the 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 there is no particular limitation on the method of press molding, for example, it is preferable to fill the granulated powder obtained in the granulation step S1 in a rubber mold and use a cold isostatic press (CIP: Cold Isostatic Press) that can apply high pressure. .
(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) The firing step S3 is the firing of the formed body obtained in the forming step S2 at a specific temperature and a specific time at a specific temperature rise rate in the sintering furnace , And the step of obtaining a sintered body. The firing step S3 is, for example, performed in the atmosphere of the firing furnace in the atmosphere. The method for producing a Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention also has characteristics in these firing conditions, which 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。[Rate of temperature rise] The rate of temperature rise from 700°C to a specific sintering temperature in the sintering furnace is preferably at a rate of 0.3 to 1.0°C/min to sinter the molded body. It has the effect of promoting the diffusion of ZnO, SnO 2 or Zn 2 SnO 4 compounds, improving sinterability, and improving conductivity. In addition, by setting such a heating rate, it also has the effect of suppressing the volatilization of ZnO or Zn 2 SnO 4 in the high temperature range.
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 of manufacturing a Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention, SnO 2 may also be present during sintering (lower temperature range), but Sn/(Zn+ Sn) is 0.1 or more and 0.3 or less. If the sintering at the specified temperature is completed, the SnO 2 phase will disappear, 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)。When the heating rate in the sintering furnace is less than 0.3°C/min, the diffusion of the compound will decline. In addition, if it exceeds 1.0° C./min, since the rate of temperature rise is rapid, compound formation may be incomplete, and a dense sintered body cannot be produced. (Refer to 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 more and 1400°C or less. When the sintering temperature is less than 1300°C (refer to Comparative Example 5), the temperature will be too low, and the sintering grain boundary diffusion in the ZnO, SnO 2 , and Zn 2 SnO 4 compounds does not proceed. On the other hand, even when it exceeds 1400°C (see Comparative Example 6), although grain boundary diffusion is promoted and sintering proceeds, volatilization of the Zn component cannot be suppressed, and a large number of pores 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)。[Holding time] The holding time is preferably set to 15 hours or more and within 25 hours. If it is less than 15 hours, the sintering will be incomplete, so it becomes a sintered body with large deformation or warpage, and grain boundary diffusion does not proceed, and sintering does not proceed. As a result, a dense sintered body could not be produced (see Comparative Example 7). On the other hand, if it exceeds 25 hours, the volatilization of ZnO or Zn 2 SnO 4 will increase, resulting in a decrease in density, deterioration of 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 of one embodiment of the present invention having Zn and Sn as main components obtained under such conditions also has improved conductivity, and therefore becomes a film that can be formed by DC sputtering. In addition, since no special manufacturing method is used, it can also be applied to cylindrical targets. [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 explained in more detail using examples, but the present invention is not limited at all by 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, SnO 2 powder, ZnO powder, GeO 2 powder as the first additional element Ge, Ta 2 O 5 powder as the second additional element Ta, and Ga as the third additional element were prepared The 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, SnO 2 powder and ZnO powder are blended so that the atomic ratio of Sn to Zn Sn/(Sn+Zn) becomes 0.2, so that the atomic ratio of the first additional element Ge is Ge/(Sn+Zn+Ge +Ta+Ga) becomes 0.004, the atomic ratio Ta/(Sn+Zn+Ge+Ta+Ga) of the second additional element Ta is 0.002, and the atomic ratio of the third additional element Ga Ga/((Sn +Zn+Ge+Ta+Ga) becomes 0.02 to prepare 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, pure water or ultrapure water, organic binder, dispersant, and defoamer are mixed in a mixing tank so that the concentration of the raw material powder becomes 55-65% by mass. Next, using a bead mill (made by Ashizawa Finetech Co., Ltd., LMZ type) into which hard ZrO 2 balls were introduced, wet pulverization was performed until the average particle size of the raw material powder became 1 μm or less, and then mixed and stirred for more than 10 hours to obtain a slurry body. In addition, in order to measure the average particle size of the raw material powder, a laser diffraction particle size distribution measuring device (manufactured by Shimadzu Corporation, SALD-2200) 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 sprayed and dried with a spray drying device (manufactured by Okawara Chemical Industry 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。Then, the obtained granulated powder was filled in a rubber mold, and a pressure of 294 MPa (3 ton/cm 2 ) was applied by cold equalization to form. The obtained formed body with a diameter of about 250 mm was put into an atmospheric sintering furnace and placed in the sintering furnace. Introduce air to 700°C. After confirming that the temperature in the firing furnace became 700°C, oxygen was introduced, the temperature was raised to 1350°C, and the temperature was maintained at 1350°C for 20 hours. The heating rate at this time is 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 end of the holding time, the introduction of oxygen was stopped and cooling was performed, and the Sn-Zn-O-based oxide sintered body of Example 1 was obtained.
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 (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 Archimedes' method, the relative density is 99.0%. In addition, the specific resistance measured by the four-probe method was 5.5Ω・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 the processed body was cut and crushed with a mortar to form a powder. For this powder, the result of analysis using an X-ray diffraction device [X'Pert-PRO (manufactured by PANalytical)] with CuKα rays showed that the spinel crystal structure of the Zn 2 SnO 4 phase is 66% and wurtzite The ZnO phase of the mineral crystal structure is 34% diffraction of the whole, and the diffraction peaks of other compound phases are not measured. The 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 Sn and Zn atomic ratio Sn/(Sn+Zn) was prepared at a ratio of 0.1, except that the same method as in Example 1 was used to obtain an example 2 Sn-Zn-O series oxide sintered body. In the same manner as in Example 1, the powder X-ray diffraction analysis showed that 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 peaks of other compound phases were measured. In addition, the relative density is 96.0%, and the specific resistance value is 1780Ω・cm. The 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, the atomic ratio of Sn to Zn, Sn/(Sn+Zn), was blended at a ratio of 0.3, except that the same method as Example 1 was used to obtain an example 3 Sn-Zn-O series oxide sintered body. In the same manner as in Example 1, as a result of X-ray diffraction analysis of the powder, the wurtzite-type ZnO phase is 5%, and the spinel-type crystalline structure of the Zn 2 SnO 4 phase is 95% diffraction. No diffraction peaks of other compound phases were measured. In addition, the relative density is 95.5%, and the specific resistance value is 7100Ω・cm. The 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 number of Sn to Zn, Sn/(Sn+Zn) was 0.1, so that the atomic ratio of the first additional element Ge was Ge/(Sn+Zn). +Ge+Ta+Ga) becomes 0.0005, the atomic number ratio Ta/(Sn+Zn+Ge+Ta+Ga) of the second additional element Ta is 0.0005, and the atomic number ratio of the third additional element Ga Ga/( GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder were prepared so that Sn+Zn+Ge+Ta+Ga) became 0.001, except that the same method as in Example 1 was used to obtain an example 4 Sn-Zn-O series oxide sintered body. As in Example 2, the wurtzite type ZnO phase is 70%, and the spinel crystal structure of the Zn 2 SnO 4 phase is 30% diffraction. No diffraction peaks of other compound phases were measured. In addition, the relative density is 95.0%, and the specific resistance value is 5300Ω・cm. The 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 number of Sn to Zn, Sn/(Sn+Zn) was 0.1, so that the atomic ratio of the first additional element Ge was Ge/(Sn+Zn). +Ge+Ta+Ga) is set to 0.01, the atomic number ratio Ta/(Sn+Zn+Ge+Ta+Ga) of the second additional element Ta is set to 0.01, and the atomic number ratio of the third additional element Ga Ga/( GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder were prepared so that Sn+Zn+Ge+Ta+Ga) became 0.1, except that the same method as in Example 1 was used to obtain an example 5 Sn-Zn-O series oxide sintered body. As in Example 2, the wurtzite type ZnO phase is 70%, and the spinel crystal structure of the Zn 2 SnO 4 phase is 30% diffraction. No diffraction peaks of other compound phases were measured. In addition, the relative density is 96.0%, and the specific resistance value is 980Ω・cm. The 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 atomic ratio of Sn to Zn, Sn/(Sn+Zn) was 0.3, so that the atomic ratio of Ge as the first additional element Ge/(Sn+Zn) +Ge+Ta+Ga) becomes 0.0005, the atomic number ratio Ta/(Sn+Zn+Ge+Ta+Ga) of the second additional element Ta is 0.0005, and the atomic number ratio of the third additional element Ga Ga/( GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder were prepared so that Sn+Zn+Ge+Ta+Ga) became 0.001, except that the same method as in Example 1 was used to obtain an example 6 Sn-Zn-O series oxide sintered body. As in Example 3, the wurtzite type ZnO phase is 5%, and the spinel type crystal structure of the Zn 2 SnO 4 phase is 95% diffraction. No diffraction peaks of other compound phases were measured. In addition, the relative density is 94.7%, and the specific resistance value is 10000Ω・cm. The 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 atomic ratio of Sn to Zn, Sn/(Sn+Zn) was 0.3, so that the atomic ratio of Ge/(Sn+Zn) +Ge+Ta+Ga) is set to 0.01, the atomic number ratio Ta/(Sn+Zn+Ge+Ta+Ga) of the second additional element Ta is set to 0.01, and the atomic number ratio of the third additional element Ga Ga/( GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder were prepared so that Sn+Zn+Ge+Ta+Ga) became 0.1, except that the same method as in Example 1 was used to obtain an example 7 Sn-Zn-O series oxide sintered body. As in Example 3, the wurtzite type ZnO phase is 5%, and the spinel type crystal structure of the Zn 2 SnO 4 phase is 95% diffraction. No diffraction peaks of other compound phases were measured. In addition, the relative density is 95.0%, and the specific resistance value is 9500Ω・cm. The 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 atomic ratio of Sn to Zn, Sn/(Sn+Zn), was blended at a ratio of 0.16, and the sintering holding temperature was set to 1300°C. In the same manner as in Example 1, the Sn-Zn-O-based oxide sintered body of Example 8 was obtained. In the same manner as in Example 1, the powder X-ray diffraction analysis showed that the Zn 2 SnO 4 phase of the spinel crystal structure was 54%, and the ZnO phase of the wurtzite crystal structure was 46% of the total winding. No diffraction peaks of other compound phases were measured. In addition, the relative density is 98.0%, and the specific resistance value is 60Ω・cm. The 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 atomic ratio of Sn to Zn, Sn/(Sn+Zn), was blended at a ratio of 0.23, and the sintering holding temperature was set to 1400°C. In the same manner as in Example 1, the Sn-Zn-O-based oxide sintered body of Example 9 was obtained. In the same manner as in Example 1, the powder X-ray diffraction analysis showed that 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 total winding. No diffraction peaks of other compound phases were measured. In addition, the relative density is 98.5%, and the specific resistance value is 105Ω・cm. The 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 number of Sn to Zn, Sn/(Sn+Zn) was 0.3, so that the atomic ratio of the first additional element Ge was Ge/(Sn+Zn). +Ge+Ta+Ga) becomes 0.0005, the atomic number ratio Ta/(Sn+Zn+Ge+Ta+Ga) of the second additional element Ta is 0.0005, and the atomic number ratio of the third additional element Ga Ga/( GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder were prepared so that Sn+Zn+Ge+Ta+Ga) became 0.001, and the sintering retention time was 15 hours. In addition, the same as in Example 1 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 is 5%, and the spinel crystal structure of the Zn 2 SnO 4 phase is 95% diffraction. No diffraction peaks of other compound phases were measured. In addition, the relative density is 94.0%, and the specific resistance value is 12000Ω・cm. The 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 number of Sn to Zn, Sn/(Sn+Zn) was 0.3, so that the atomic ratio of the first additional element Ge was Ge/(Sn+Zn). +Ge+Ta+Ga) is set to 0.01, the atomic number ratio Ta/(Sn+Zn+Ge+Ta+Ga) of the second additional element Ta is set to 0.01, and the atomic number ratio of the third additional element Ga Ga/( GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder were prepared so that Sn+Zn+Ge+Ta+Ga) became 0.1, and the sintering retention time was 25 hours. In addition, the same as in Example 1 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 is 5%, and the spinel type crystal structure of the Zn 2 SnO 4 phase is 95% diffraction. No diffraction peaks of other compound phases were measured. In addition, the relative density is 95.5%, and the specific resistance value is 10500Ω・cm. The 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 number of Sn to Zn, Sn/(Sn+Zn) was 0.1, so that the atomic ratio of the first additional element Ge was Ge/(Sn+Zn). +Ge+Ta+Ga) is set to 0.01, the atomic number ratio Ta/(Sn+Zn+Ge+Ta+Ga) of the second additional element Ta is set to 0.01, and the atomic number ratio of the third additional element Ga Ga/( Sn+Zn+Ge+Ta+Ga) becomes 0.1 to prepare GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder, and set the heating rate to 0.3°C/min. In the same manner as in Example 1, the Sn-Zn-O-based oxide sintered body of Example 12 was obtained. As in Example 2, the wurtzite type ZnO phase is 70%, and the spinel crystal structure of the Zn 2 SnO 4 phase is 30% diffraction. No diffraction peaks of other compound phases were measured. In addition, the relative density is 95.0%, and the specific resistance value is 1320Ω・cm. The 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 atomic ratio of Sn to Zn, Sn/(Sn+Zn) was 0.1, so that the atomic ratio of Ge/(Sn+Zn) as the first additive element +Ge+Ta+Ga) becomes 0.0005, the atomic number ratio Ta/(Sn+Zn+Ge+Ta+Ga) of the second additional element Ta is 0.0005, and the atomic number ratio of the third additional element Ga Ga/( GeO 2 powder, Ta 2 O 5 powder, and Ga 2 O 3 powder are prepared so that Sn+Zn+Ge+Ta+Ga) becomes 0.001, and the heating rate is set to 1.0°C/min. In the same manner as in Example 1, the Sn-Zn-O-based oxide sintered body of Example 13 was obtained. As in Example 2, the wurtzite type ZnO phase is 70%, and the spinel crystal structure of the Zn 2 SnO 4 phase is 30% diffraction. No diffraction peaks of other compound phases were measured. In addition, the relative density is 94.5%, and the specific resistance value is 6800Ω・cm. The 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, the ratio of the atomic number of Sn to Zn, Sn/(Sn+Zn), was 0.05. Except that, the comparative example was obtained in the same manner as in Example 1. 1 Sn-Zn-O series oxide sintered body. With regard to the Sn-Zn-O-based oxide sintered body of Comparative Example 1, the results of X-ray diffraction analysis performed in the same manner as in Example 1 showed that the wurtzite-type ZnO phase is 90% and the spinel-type crystal structure is The Zn 2 SnO 4 phase is 10% diffraction. No diffraction peaks of other compound phases were measured. In addition, as a result of measuring the relative density and the specific resistance value, the relative density was 93.0%, and the specific resistance value was 3510Ω・cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5Ω・cm or more and 12000Ω・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, the ratio of the atomic number of Sn to Zn, Sn/(Sn+Zn) was 0.40, and except that the ratio was prepared in the same manner as in Example 1, a comparative example was obtained. 2 Sn-Zn-O series oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 2, the results of X-ray diffraction analysis in the same manner as in Example 1 showed that the wurtzite-type ZnO phase was 0% and the rutile-type SnO 2 phase was 14 %, and the spinel crystal structure of Zn 2 SnO 4 phase is 86% diffraction. No diffraction peaks of other compound phases were measured. In addition, as a result of measuring the relative density and the specific resistance value, the relative density was 89.0%, and the specific resistance value was 597000Ω・cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5Ω・cm or more and 12000Ω・cm or less could not be achieved. 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) In Comparative Example 3, except that the heating rate was set to 0.2°C/min, the Sn-Zn-O-based oxide sintered body of Comparative Example 3 was obtained in the same manner as in Example 1 . With regard to the Sn-Zn-O-based oxide sintered body of Comparative Example 3, the results of X-ray diffraction analysis performed in the same manner as in Example 1 showed that the wurtzite-type ZnO phase is 34% and the spinel-type crystal structure is The Zn 2 SnO 4 phase is 66% diffraction. No diffraction peaks of other compound phases were measured. Also, as a result of measuring the relative density and the specific resistance value, the relative density was 90.0%, and the specific resistance value was 15000Ω・cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5Ω・cm or more and 12000Ω・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) In Comparative Example 4, except that the temperature increase rate was set to 1.2°C/min, the Sn-Zn-O-based oxide sintered body of Comparative Example 4 was obtained in the same manner as in Example 1 . With regard to the Sn-Zn-O-based oxide sintered body of Comparative Example 4, the result of X-ray diffraction analysis performed in the same manner as in Example 1 showed that the wurtzite-type ZnO phase is 34%, and the spinel-type crystal structure is The Zn 2 SnO 4 phase is 66% diffraction. No diffraction peaks of other compound phases were measured. In addition, as a result of measuring the relative density and the specific resistance value, the relative density was 92.0%, and the specific resistance value was 12500Ω・cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5Ω・cm or more and 12000Ω・cm or less could not be achieved. 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) In Comparative Example 5, except that the sintering temperature was 1280° C., in the same manner as in Example 1, a Sn-Zn-O-based oxide sintered body of Comparative Example 5 was obtained. For the Sn-Zn-O-based oxide sintered body of Comparative Example 5, the results of X-ray diffraction analysis performed in the same manner as in Example 1 showed that the wurtzite-type ZnO phase is 34%, and the spinel-type crystal structure is The Zn 2 SnO 4 phase is 66% diffraction. No diffraction peaks of other compound phases were measured. In addition, as a result of measuring the relative density and the specific resistance value, the relative density was 91.0%, and the specific resistance value was 14000Ω・cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5Ω・cm or more and 12000Ω・cm or less could not be achieved. 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) In Comparative Example 6, except that the sintering temperature was set to 1430°C, in the same manner as in Example 1, a Sn-Zn-O-based oxide sintered body of Comparative Example 6 was obtained. With regard to the Sn-Zn-O-based oxide sintered body of Comparative Example 6, X-ray diffraction analysis was 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% diffraction. No diffraction peaks of other compound phases were measured. In addition, as a result of measuring the relative density and the specific resistance value, the relative density was 93.0%, and the specific resistance value was 12500Ω・cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5Ω・cm or more and 12000Ω・cm or less could not be achieved. 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, the retention time of sintering at 1350°C was set to 10 hours, except that the Sn-Zn-O system of Comparative Example 7 was obtained in the same manner as in Example 1. Oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 7, X-ray diffraction analysis was 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% diffraction. No diffraction peaks of other compound phases were measured. Also, as a result of measuring the relative density and the specific resistance value, the relative density was 90.0%, and the specific resistance value was 13500Ω・cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5Ω・cm or more and 12000Ω・cm or less could not be achieved. 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 retention time of sintering at 1350°C was 30 hours. Oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 8, X-ray diffraction analysis was 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% diffraction. No diffraction peaks of other compound phases were measured. In addition, as a result of measuring the relative density and specific resistance, ZnO or Zn 2 SnO 4 was volatilized, and the relative density was 93.0%, and the specific resistance was 13000Ω・cm. That is, it was confirmed that a relative density of 94% or more and a specific resistance of 5Ω・cm or more and 12000Ω・cm or less could not be achieved. 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) In Comparative Example 9, the ratio of Ge/(Sn+Zn+Ge+Ta+Ga) was 0.03, except that it was the same as Example 1, and Comparative Example 9 was obtained. The Sn-Zn-O series oxide sintered body. With regard to the Sn-Zn-O-based oxide sintered body of Comparative Example 9, the results of X-ray diffraction analysis performed in the same manner as in Example 1 showed that the wurtzite-type ZnO phase is 34%, and the spinel-type crystal structure is The Zn 2 SnO 4 phase is 66% diffraction. No diffraction peaks of other compound phases were measured. In addition, as a result of measuring the relative density and the specific resistance value, the relative density was 93.0%, and the specific resistance value was 8500Ω・cm. That is, it was confirmed that a relative density of 94% or more could not be achieved. 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) In Comparative Example 10, the ratio of Ge/(Sn+Zn+Ge+Ta+Ga) was 0.0001, except that it was the same as in Example 1, and Comparative Example 10 was obtained. The Sn-Zn-O series oxide sintered body. With regard to the Sn-Zn-O based oxide sintered body of Comparative Example 10, the results of X-ray diffraction analysis performed in the same manner as in Example 1 showed that the wurtzite-type ZnO phase is 34%, and the spinel-type crystal structure is The Zn 2 SnO 4 phase is 66% diffraction. No diffraction peaks of other compound phases were measured. In addition, as a result of measuring the relative density and the specific resistance value, the relative density was 91.0%, and the specific resistance value was 9800Ω・cm. That is, it was confirmed that a relative density of 94% or more could not be achieved. 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) In Comparative Example 11, except that the ratio of Ta/(Sn+Zn+Ge+Ta+Ga) was 0.03, it was prepared in the same manner as in Example 1, and Comparative Example 11 was obtained. The Sn-Zn-O series oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 11, X-ray diffraction analysis was 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% diffraction. No diffraction peaks of other compound phases were measured. Furthermore, as a result of measuring the relative density and the specific resistance value, the relative density was 97.0%, and the specific resistance value was 16000Ω・cm. That is, it was confirmed that the specific resistance could not be achieved at 5Ω・cm or more and 12000Ω・cm or less. 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) In Comparative Example 12, the ratio of Ta/(Sn+Zn+Ge+Ta+Ga) was 0.0001, except that it was prepared in the same manner as in Example 1, and Comparative Example 12 was obtained. The Sn-Zn-O series oxide sintered body. For the Sn-Zn-O based oxide sintered body of Comparative Example 12, X-ray diffraction analysis was 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% diffraction. No diffraction peaks of other compound phases were measured. In addition, as a result of measuring the relative density and the specific resistance value, the relative density was 96.7%, and the specific resistance value was 25000Ω・cm. That is, it was confirmed that the specific resistance could not be achieved at 5Ω・cm or more and 12000Ω・cm or less. 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) In Comparative Example 13, the ratio of Ga/(Sn+Zn+Ge+Ta+Ga) was 0.2. Except that, in the same manner as in Example 1, Comparative Example 13 was obtained. The Sn-Zn-O series oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 13, X-ray diffraction analysis was 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% diffraction. No diffraction peaks of other compound phases were measured. Also, as a result of measuring the relative density and the specific resistance value, the relative density was 97.3%, and the specific resistance value was 14800Ω・cm. That is, it was confirmed that the specific resistance could not be achieved at 5Ω・cm or more and 12000Ω・cm or less. 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) In Comparative Example 14, Ga/(Sn+Zn+Ge+Ta+Ga) was prepared at a ratio of 0.0008. In the same manner as in Example 1, except that Ga/(Sn+Zn+Ge+Ta+Ga) was blended, Comparative Example 14 was obtained. The Sn-Zn-O series oxide sintered body. For the Sn-Zn-O-based oxide sintered body of Comparative Example 14, X-ray diffraction analysis was 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% diffraction. No diffraction peaks of other compound phases were measured. Furthermore, as a result of measuring the relative density and the specific resistance value, the relative density was 97.0%, and the specific resistance value was 22000Ω・cm. That is, it was confirmed that the specific resistance could not be achieved at 5Ω・cm or more and 12000Ω・cm or less. 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. However, various modifications that do not actually deviate from the novel matters and effects of the present invention can be easily understood by the industry. 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 the specification or the drawings, the terms that are recorded at least once with the broader or synonymous different terms can be replaced with the different terms anywhere in the specification or the drawings. In addition, the structure of the Sn-Zn-O-based oxide sintered body and its manufacturing method are not limited to those described in one embodiment of the present invention and each example, and various modifications can be implemented.
[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 step diagram showing the outline of the manufacturing process of a method of manufacturing a Sn-Zn-O-based oxide sintered body according to an embodiment of the present invention.
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