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TW200923973A - Indium oxide transparent conductive film and manufacturing method thereof - Google Patents

Indium oxide transparent conductive film and manufacturing method thereof Download PDF

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Publication number
TW200923973A
TW200923973A TW097138475A TW97138475A TW200923973A TW 200923973 A TW200923973 A TW 200923973A TW 097138475 A TW097138475 A TW 097138475A TW 97138475 A TW97138475 A TW 97138475A TW 200923973 A TW200923973 A TW 200923973A
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Taiwan
Prior art keywords
film
transparent conductive
conductive film
annealing
amorphous
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TW097138475A
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Chinese (zh)
Inventor
Seiichiro Takahashi
Norihiko Miyashita
Makoto Ikeda
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Mitsui Mining & Amp Smelting Co Ltd
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Publication of TW200923973A publication Critical patent/TW200923973A/en

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    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/06Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the coating material
    • C23C14/08Oxides
    • C23C14/086Oxides of zinc, germanium, cadmium, indium, tin, thallium or bismuth

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  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • Mechanical Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Physical Vapour Deposition (AREA)
  • Compositions Of Oxide Ceramics (AREA)
  • Manufacturing Of Electric Cables (AREA)
  • Non-Insulated Conductors (AREA)

Abstract

This invention provides a transparent conductive film, using indium oxide target having a sintered oxide to form an amorphous film, wherein the sintered oxide contains indium oxide and tin, and also contains barium; wherein the content of tin and barium is such that when y represents a molar ratio of tin with respect to 1 mole of indium, and x represents a molar ratio of barium with respect to 1 mole of indium, the value of y is not reach the value of (-2.9x10<SP>-2</SP>Ln(x)-6.7x10<SP>-2</SP>).

Description

200923973 _ 六、發明說明: 【發明所屬之技術領域】 本發明係關於可成膜為非晶型膜,該非晶型膜藉由弱 酸I虫刻,進一步可容易地結晶化,再者進一步地經結晶化200923973 _ VI. Description of the Invention: [Technical Field] The present invention relates to a film which can be formed into an amorphous film which can be easily crystallized by weak acid I, and further Crystallization

I 之膜為低電阻且穿透率高之透明導電膜及其製造方法。 【先前技術】 氧化銦-氧化錫(In2〇3-Sn〇2之複合氧化物,以下稱作 「ΙΤ0」)膜由於可見光穿透性高,且導電性高,當作透明 導電膜廣泛地使用於液晶顯示裝置或玻璃之防止結露用發 ' 熱膜、紅外線反射膜等,但是有難以作成非晶型膜的問題。 另一方面,非晶型膜所成者而言,氧化銦-氧化鋅(ΙΖ0) 透明導電膜是眾所周知,但是,該膜比ΙΤ0膜之透明性差, 為帶有黃色狀態問題。 因此,本發明之申請者先前提案作為透明導電膜係於 ΙΤ0中添加矽,以規定條件成膜非晶型之透明導電膜(參照 專利文獻1) 5但是’添加石夕時有面電阻化傾向的問題。 [專利文獻1]日本特開2005-135649公報(申請專利範圍)。 【發明内容】 [發明欲解決之課題] 本發明乃鑑於此等問題,提供可成膜為非晶型膜,該 非晶型膜藉由弱酸蝕刻可容易地圖案化,進一步可容易地 結晶化,再者進一步地經結晶化之膜為低電阻且穿透率高 之透明導電膜及其製造方法當作課題。 [解決課題之方法] 320646 200923973 ‘ 树明是為解決上述課題進行各種檢討之結果,得知 經,加鋇之氧化銦系透明導電膜為低電阻且透明性優異之 非^曰型膜,藉由弱酸蚀刻可容易地圖案化,再者進一步地 ’可合易地紇日日化,而先提出申請(日本特願2007-095783)。 於該况下,關於結晶化溫度為1〇〇。〇以下之組成範 圍’成膜為非晶型膜為條件極嚴苛的課題,本發明乃係解 決相關課題者。 f 、關於本發明第1態樣為使料備氧化物燒結體之濺鐘 靶成膜為非晶型膜的透明導電膜,該氧化物燒結體含有氧 化口與錫及同時含有鋇,該透明導電膜之特徵為含有氧化 鋼與錫及同時含有鋇,*且㈣独1莫耳之錫的莫耳比 y =目對於銦1莫耳之鋇的莫耳比以χ表示時為未達(_2.9 。1〇 Ln(x) 6. 7xl〇2)之值’藉由退火之結晶化溫度為 C以上。 ^於發明第1態樣巾,藉由含有錫錢之規定組成範 i 的軋化銦系透明導電膜’比較容易地成膜為非晶型膜, 且使以弱酸性姓刻劑之钕刻成為可能。 本發明之第2態樣係於第1態樣所述之透明導電膜 中於水的分壓為h 0xl『4Pa β上、1. Οχιό-%以下之條 件下成膜為其特徵之透明導電膜。 相關第2態樣中,藉由於規定之水的分壓下成膜,較 易方'田作非晶型臈實施成膜’比較容易地成膜為非晶型 膜’且使以弱酸性㈣劑之㈣成為可能。 本發明之第3態樣係於第1或第2之態樣所述之透明 4 320646 200923973 導電膜中’前述之非晶型膜含有氫為其特徵之透明導電膜。 相關第3態樣中,藉由於規定之水的分壓下成膜,氣 是以結合於膜内的狀態取入,比較容易地成膜為非晶型 膜’且使以弱酸性蝕刻劑之蝕刻成為可能。 本發明之第4態樣係於第1至3之任一態樣中所述之 透明導電膜,成膜後藉由退火而成結晶化膜為其特徵之透 明導電膜。 相關第4態樣中,係成膜為非晶型膜後,可藉由退火 容易地結晶化,可賦予抗弱酸性。 本發明之» 5態樣係於第4態'樣所述之透明導電月 中,前述退火於100至300t:進行為其特徵之透明導電^ 相關第4態樣中,是以較低溫度結晶化之膜。、 電膜樣係於第4或第5態樣所述之透, 電財,退火後之透明導電膜的電阻率為 , 以下為其特徵之透明導電膜。 . 相關以態樣中,退火後之電阻率非常低,The film of I is a transparent conductive film having low resistance and high transmittance and a method for producing the same. [Prior Art] Indium oxide-tin oxide (composite oxide of In2〇3-Sn〇2, hereinafter referred to as "ΙΤ0") film is widely used as a transparent conductive film because of its high visible light transmittance and high conductivity. In the liquid crystal display device or the glass, the heat-preventing film, the infrared-ray reflective film, and the like are prevented from being dew condensation, but there is a problem in that it is difficult to form an amorphous film. On the other hand, an indium oxide-zinc oxide (ITO) transparent conductive film is well known as an amorphous film. However, this film is inferior in transparency to the ΙΤ0 film and has a yellow state problem. Therefore, the applicant of the present invention has previously proposed to add a ruthenium to ΙΤ0 as a transparent conductive film, and to form a transparent transparent conductive film under predetermined conditions (see Patent Document 1). The problem. [Patent Document 1] Japanese Laid-Open Patent Publication No. 2005-135649 (Application No.). SUMMARY OF THE INVENTION [Problems to be Solved by the Invention] In view of the above problems, the present invention provides a film which can be formed into an amorphous film which can be easily patterned by weak acid etching and further crystallized easily. Further, the film which is further crystallized is a transparent conductive film having low resistance and high transmittance, and a method for producing the same. [Means for Solving the Problem] 320646 200923973 'Shu Ming is the result of various reviews to solve the above problems. It is known that the indium oxide-based transparent conductive film which is added is a low-resistance and excellent transparency. It can be easily patterned by weak acid etching, and further, it can be easily changed, and the application is made first (Japanese Patent Application No. 2007-095783). In this case, the crystallization temperature was 1 Torr. In the following composition range, the formation of an amorphous film is an extremely difficult condition, and the present invention is intended to solve related problems. f. The first aspect of the present invention is a transparent conductive film in which a sputtering target of a material oxide sintered body is formed into an amorphous film, and the oxide sintered body contains an oxide port and tin and contains germanium. The conductive film is characterized by containing oxidized steel and tin and containing yttrium, * and (d) Mohs y = y = for the indium 1 耳 钡 莫 对于 对于 铟 铟 铟 铟 铟 铟 铟 铟 铟 铟_2.9 .1〇Ln(x) 6. The value of 7xl〇2) 'The crystallization temperature by annealing is C or more. ^In the invention of the first aspect of the sample, the indium-based transparent conductive film containing the tin-containing composition of the formula i is relatively easy to form an amorphous film, and the engraving of the weakly acidic surrogate become possible. The second aspect of the present invention is a transparent conductive film characterized by forming a film under the condition that the partial pressure of water is h 0xl "4Pa β or less than 1. Οχιό-% in the transparent conductive film according to the first aspect. membrane. In the second aspect, the film is formed by partial pressure of the specified water, and it is easier to form a film into an amorphous film by using a film of the amorphous type, and the weakly acidic (four) agent is used. (4) It is possible. The third aspect of the present invention is in the transparent film of the first or second aspect of the present invention. The above-mentioned amorphous film contains a transparent conductive film characterized by hydrogen. In the third aspect, the film is formed by a partial pressure of water, and the gas is taken in a state of being bonded to the film, and the film is relatively easily formed into an amorphous film and the weakly acidic etchant is used. Etching is possible. The fourth aspect of the present invention is the transparent conductive film described in any one of the first to third aspects, and the transparent conductive film characterized by annealing to form a crystallized film. In the fourth aspect, after the film formation is an amorphous film, it can be easily crystallized by annealing, and the weak acidity can be imparted. The +5 aspect of the present invention is in the transparent conductive month of the fourth state, and the annealing is performed at 100 to 300 t: the transparent conductive characteristic is characterized by the fourth aspect, which is crystallized at a lower temperature. Membrane. The electro-membrane pattern is a transparent conductive film characterized by the conductivity of the transparent conductive film after permeation, electricity, and annealing described in the fourth or fifth aspect. In the relevant aspect, the resistivity after annealing is very low.

卞為5. GxlG 4Q . on以下的低電阻膜。 _ ”'、电PJ 本發明之第7態樣係透明導電膜 1 備氧化物燒結體之濺鍍靶,該氣、衣&amp;方法,使用具 錫及同時含有鋇,該透明導電膜之特二 =有氧化銦與 且同時含有鋇,而且相對於錮為3有缝銦與錫 對於銦1莫耳之鋇的莫耳、之錫的莫耳比y:相 i〇W6.—非未達(⑼ 之分壓為l.〇xlo,a以上、1〇χΐρ '成臊蚪’成膜時的水 广3以下。 320646 200923973 相關第7態樣中’藉由於規定之水的分壓下成膜含有 鋇,規疋組成的氧化銦系透明導電膜,比較容易地成膜為 非曰B型膜,且使以弱酸性蝕刻劑之蝕刻成為可能。 ,本發明之第8態樣係於第7態樣所述的透明導電膜之 。衣l方法中,岫述非晶型膜之藉由退火的結晶化溫度為1〇〇 C以上為其特徵之透明導電膜。 相關第8態樣中,由於為結晶化溫度100DC以上所成卞 is a low resistance film of 5. GxlG 4Q . _"', electric PJ The seventh aspect of the present invention is a transparent conductive film 1 prepared by sputtering a target of an oxide sintered body, the gas, clothing &amp; method, using tin and containing yttrium, the transparent conductive film Two = with indium oxide and at the same time containing yttrium, and relative to yttrium 3 with a slit of indium and tin for indium 1 Mo, the molar ratio of tin to y: phase i 〇 W6. - non-deficient ((9) The partial pressure is l.〇xlo, a or more, 1〇χΐρ '成臊蚪', and the water is 3 or less at the time of film formation. 320646 200923973 In the seventh aspect, 'by the specified partial pressure of water The film contains an indium oxide-based transparent conductive film having a ruthenium composition, and is relatively easy to form a non-曰B-type film, and etching with a weakly acidic etchant is possible. The eighth aspect of the present invention is based on In the method of the first embodiment, the transparent conductive film characterized by annealing at a crystallization temperature of 1 〇〇 C or more is described in the coating method. Due to the crystallization temperature of 100DC or more

g曰曰i膜,比較谷易地成膜為非晶型膜,且使以弱酸性 蝕刻劑之蝕刻成為可能。 “本2明之第9態樣係於第7或第8態樣所述之透明導 電膜之衣1^方法中,成膜為非晶型膜後,藉由退火而 晶化膜為其特徵之透明導電膜之製造方法。 、’° —相關的第9態樣中,成膜為非晶型膜後,藉由退 容易地結晶化,可賦予抗弱酸性。 本發月之第1Q ‘%樣係於第9態樣所述之透明導電膜 衣造方法中,前述藉由退火而έ士曰介1nn 、、 — 泪、人肉'、‘口日日化係於100至3〇〇它進 仃為其彳寸徵之透明導電膜的製造方法。 相關第10態樣中 結晶化膜。 ,是於100至30(TC之比較低溫而成 本發明之第n態樣係於第1()態樣所述之 的製造方法中,迖火铉夕'φ曾 ¥電族 、火後之透明V電膜的電阻率為5 cnm下為其特徵之透明導電膜的製造方法。 =11態樣中’退火後之電阻率非常低,可為電阻 千5. 0x10 Ω . cm以下之低電阻膜。 ”、、电 320646 6 200923973 - [發明之效果] 根據本發明,藉由以氧化銦中添加錫及鋇之膜具有規 定範圍之組成,且具有規定之結晶化溫度而成之非晶型 ,膜,可比較容易地成為非晶型膜,成膜後,可藉由弱酸蝕 刻劑容易地圖案化,進一步可容易地結晶化,再者進一步 地經結晶化之膜可顯示低電阻且穿透率高的透明導電性膜 之效果。 【實施方式】 為形成本發明的氧化銦系透明導電膜所使用之透明導 電膜用濺鍍靶,乃係以氧化銦為主體,為含有錫且含有鋇 之氧化物燒結體,鋇以氧化物之原樣,或是複合氧化物之 方式,或是以固溶體之方式存在皆可,並無特別限制。 鋇的含有量,希望使用含有相對於銦1莫耳為0. 00001 莫耳以上且未達0. 10莫耳之範圍之藏鍵乾形成為佳。添加 量較此含有量少時,則無明顯的添加效果,再者較此添加 , 量多時,則所形成透明導電膜之電阻有變高之傾向及帶黃 色狀況更惡化的傾向。再者,根據上述之藏鑛#巴所形成的 透明導電膜中之鋇含有量,與所使用的濺鍍靶中的含有量 相同。 再者,錫的含有量,期望使用含有相對於銦1莫耳為 0. 001至0. 3莫耳,較佳為0. 005至0. 3莫耳之範圍之濺 鍍萆巴成膜為佳。若在此範圍内,適當地控制藏鍍革巴之載體 電子的密度及移動度,可於良好範圍保持導電性。再者, 若添加超過此範圍的量時,由於致使濺鍍靶之載體電子的 7 320646 200923973 - 移動度降低’同時讓導電性移往惡化的方向,故不理想。 又’根據上述濺鍍靶所形成的透明導電膜中之錫的含有 量,與所使用的濺鍍靶中的含有量相同。該等氧化銦系透 . 明導電膜之組成分析,可全量溶解單膜後以ICP分析。再 &gt; 者,膜本身成為元件結構之情況時,因應所需,以FIB (Focused Ion Beam:聚焦離子束)切出該部分之剖面,亦 有可能特定使用附屬於SEM(Scanning Electron / microscope :掃描式電子顯微鏡)或TEM(穿透式電子顯微 鏡)等之元素分析儀器(EDS(能量分散方式)或WDS、[奥格 電子分光法(Auger electron spectroscopy)分析等] 相關的濺鍍靶,由於具有可以直流磁控濺鍍(DC Magnetron Sputtering)進行濺鍍之程度的電阻值,雖然有 可以比較廉價的直流磁控濺鍍進行濺鍍,當然,亦可使用 高頻率磁控藏鍍裝置。 使用此等之透明導電膜用濺鍍靶,藉由於水之分壓為 I, 1· 〇xl〇_4Pa以上、1. OxlOla下之條件下成膜,可形成相同 組成之非晶型氧化銦系透明導電膜。 此處,為使上述的水之分壓為規定範圍,可在成膜室 中於成膜時導入環境氣體(一般是氬氣,因應所需為含有氧 之氣體,例如l(T4Pa程度之壓力)且同時透過流量控制器 (mass flow controller)等導入水蒸氣即可,到達真空度 為未達l(T4Pa與高真空度之情況時,使環境氣體為ι/1〇〇 至1/10之壓力程度較佳。又,到達真空度1〇_4至l〇_3pa左 右與真空度很差的條件下,該剩餘氣體之主成分是水。亦 8 320646 200923973 - 即,因為該到達真空度是幾乎相當於水之分壓,不特別導 入水蒸氣,可得到所期望的水之分壓狀態。 此等的本發明之氧化銦系透明導電膜,由於鋇是以規 定量含有,成膜藉由於室溫以上於結晶化溫度,亦即比100 °c以上之結晶化溫度低的溫度條件進行,以非晶型狀之狀 態成膜。再者,此等之非晶型膜是具有可以弱酸性的蝕刻 劑進行蝕刻之優點。此處,本說明書中,由於蝕刻是包含 ,. 在圖案化步驟中,為可製得規定之圖案者。 再者,所製得的透明導電膜之電阻率係依照鋇之含有 量而有所差異,但是電阻率為1. 0x1 (Γ4至1. 0x1 (Γ3Ω . cm。 進一步地,成膜之膜的結晶化溫度依照鋇之含有量而 有所差異,含有量愈提升,結晶化溫度就隨之提升,但藉 由於100°C至300°C之溫度條件退火,可使其結晶化。由於 此等溫度領域為通常半導體製造步驟所使用者,亦可於此 等步驟中使其結晶化。又,於此溫度範圍中,以1 oo°c至 k 300°C結晶化為佳,以15〇r至250t:結晶化為較佳,以200 °匚至250°C結晶化為最佳。 此處,退火是於大氣中、環境氣體中、真空中等,以 所希望的溫度、一定的時間加熱。所謂一定時間,一般是 從數分鐘至數小時左右,但於工業上,若效果是相同者, 短的時間為佳。 此處,本發明之透明導電膜,使用濺鍍靶之組成範圍 為相對於銦1莫耳之錫的莫耳比y,相對於銦1莫耳鋇之 莫耳比以X表示為未達(-2. 9xl(T2Ln(x)-6. 7χ1(Γ2)之值,藉 9 320646 200923973 h OxlOla以下的條件 l〇〇°C左右,可製得非 由於水之分壓為l.〇xl〇-4Pa以上、 成膜,提高少許成膜溫度,設定於 晶型膜。 l^u 疋企3成膜為非晶型听,%須如上述方式於 膜之膜的組成於較結晶化溫度更低的成膜温度成膜,錫或 ,之含有量愈少的組成則結晶化溫度愈低,錫或鋇之 量愈多的組成則結晶化溫度愈高之傾向,藉由水之分 1. 〇xl〇-4Pa以上、h 0xl0-】Pa以下之條件下成膜與水:分 = 成膜時相比較’各組成的結晶 至⑽。C左右。因此,相對於銦^耳之錫 n(x) 6.7xl〇 )之值的組成範圍時,於 ,u&gt;arPa成膜時之結晶化溫度未達靴,特別= 了製得非晶型膜之成膜條件是 ,藉 使:之分壓為l〇x10、以上、&quot;xl〇_ipa 成膜條件可製得非^副…,例如以靴左右之 晶化:产水:分壓比h崎更低時,提升如上述之結 Μ〇-%)=,=顯士的效果,另一方面,水的分壓比上限(1 ·0 而結 、士月況時’所製得的膜雖為非晶型,但是,退火 心I。2 ’膜的比電阻(電阻率)並未降低,多數製得 电阻5.^ Ω·_下之結晶化·不佳。 再且’相對於銦〗莫耳 + 莫耳之鋇的莫耳比以γ 旲 ’相對於们 x 表不為(~2. 9χ1〇Λη(χ)-6. 7χ1(Γ2)The g曰曰i film is comparatively easy to form a film into an amorphous film, and etching with a weakly acidic etchant is possible. The ninth aspect of the present invention is based on the method of coating a transparent conductive film according to the seventh or eighth aspect. After the film is formed into an amorphous film, the film is characterized by annealing. In the ninth aspect of the related art, the film is formed into an amorphous film, and then it is easily crystallized by retreat, thereby imparting weak acid resistance. The first Q'% of the month of the month In the method of fabricating a transparent conductive film according to the ninth aspect, the above-mentioned annealing is performed by a gentleman 1 nt, a tear, a human flesh, and a mouth-to-day system at 100 to 3 〇〇.制造 制造 仃 之 。 。 。 。 。 。 。 。 。 。 。 。 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 相关 结晶 相关 结晶In the manufacturing method as described above, the method of manufacturing a transparent conductive film characterized by a resistivity of a transparent V-electrode film of a group of volts and volts is 5 cnm. 'The resistivity after annealing is very low, and it can be a low-resistance film with a resistance of 5.00x10 Ω.cm or less.",, electric 320646 6 200923973 - [Effect of the invention] According to the present invention In the case where a film having a predetermined range of a film of tin and antimony added to indium oxide and having a predetermined crystallization temperature is formed, the film can be relatively easily formed into an amorphous film, and after film formation, It can be easily patterned by a weak acid etchant, and can be easily crystallized, and further, the crystallized film can exhibit the effect of a transparent conductive film having low electrical resistance and high transmittance. The sputtering target for a transparent conductive film used in the indium oxide-based transparent conductive film of the present invention is mainly composed of indium oxide, and is an oxide sintered body containing tin and containing cerium, or as an oxide, or as a composite. O. Moss or more and less than 0. 10 Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo Mo It is better to form the key dryness in the range of the ear. When the amount of addition is less than this content, there is no obvious additive effect, and when added in a larger amount, the resistance of the transparent conductive film formed tends to become higher. And with a yellower condition Further, the content of ruthenium in the transparent conductive film formed by the above-mentioned sag #巴 is the same as the content of the sputtering target used. Further, the content of tin is desirably used.约至0. 3摩尔, preferably 0. 005 to 0. 3 moles of the range of sputtering 萆 成 film formation is better. If within this range, properly controlled The density and mobility of the carrier electrons of the Tibetan leather can maintain the conductivity in a good range. Moreover, if the amount exceeding this range is added, the carrier electrons of the sputtering target are lowered by 7 320646 200923973 - the mobility is lowered' At the same time, the conductivity is shifted to the direction of deterioration, which is not preferable. Further, the content of tin in the transparent conductive film formed by the sputtering target is the same as the content of the sputtering target used. The indium oxide is transparent. The composition of the conductive film can be analyzed by ICP after the single film is completely dissolved. Further, when the film itself becomes a component structure, the section of the portion is cut out by FIB (Focused Ion Beam) as needed, and it is also possible to use the SEM (Scanning Electron / microscope: Elemental analysis instruments such as scanning electron microscopes or TEMs (transmission electron microscopes) (EDS (energy dispersion method) or WDS, [Auger electron spectroscopy analysis, etc.] related sputtering targets due to It has a resistance value that can be sputtered by DC Magnetron Sputtering. Although there is a relatively inexpensive DC magnetron sputtering for sputtering, it is of course possible to use a high-frequency magnetron plating device. Such a transparent conductive film is formed by sputtering a target, and an amorphous indium oxide system having the same composition can be formed by forming a film under the conditions of water partial pressure of I, 1·〇xl〇_4Pa or more under 1. OxlOla. Here, in order to make the above partial pressure of water into a predetermined range, it is possible to introduce an ambient gas (generally argon gas) in the film forming chamber at the time of film formation, and it is necessary to use a gas containing oxygen as needed. l (T4Pa pressure) and simultaneously introduce water vapor through a mass flow controller, etc., when the vacuum is less than 1 (T4Pa and high vacuum, make the ambient gas ι/1〇) The pressure of 〇 to 1/10 is better. In addition, under the condition that the degree of vacuum is about 1〇_4 to l〇_3pa and the degree of vacuum is very poor, the main component of the remaining gas is water. Also 8 320646 200923973 - ie Since the degree of vacuum reached is almost equivalent to the partial pressure of water, water vapor is not particularly introduced, and a desired partial pressure state of water can be obtained. The indium oxide-based transparent conductive film of the present invention is regulated by In the amount of film formation, the film formation is carried out in a state of an amorphous state by a temperature condition at room temperature or higher at a crystallization temperature, that is, a crystallization temperature lower than 100 ° C. Further, such a film is amorphous. The film is an advantage of being etched with an etchant which can be weakly acidic. Here, in the present specification, since etching is included, in the patterning step, a predetermined pattern can be obtained. The resistivity of the transparent conductive film is in accordance with The content varies depending on the content, but the specific resistance is 1. 0x1 (Γ4 to 1. 0x1 (Γ3Ω. cm. Further, the crystallization temperature of the film formed varies depending on the content of the ruthenium, and the content is increased. The crystallization temperature is increased, but it can be crystallized by annealing at a temperature of 100 ° C to 300 ° C. Since these temperature fields are users of conventional semiconductor manufacturing steps, such steps can also be used. It is crystallized in the temperature range. In this temperature range, crystallization is preferably carried out at 1 oo ° c to k 300 ° C, preferably 15 Torr to 250 ton: crystallization is preferably carried out at 200 ° 匚 to 250 ° C. Crystallization is optimal. Here, the annealing is performed at a desired temperature and for a certain period of time in the atmosphere, in an ambient gas, or in a vacuum. The so-called certain time is usually from a few minutes to a few hours, but in the industry, if the effect is the same, a short time is better. Here, in the transparent conductive film of the present invention, the composition range using the sputtering target is the molar ratio y with respect to the tin of the indium 1 mole, and the molar ratio with respect to the indium 1 moir is expressed as X. -2. 9xl(T2Ln(x)-6. 7χ1(Γ2) value, by 9 320646 200923973 h OxlOla the following conditions l〇〇 °C or so, can be obtained due to water partial pressure is l.〇xl〇 -4Pa or more, film formation, increase the film formation temperature, and set it on the crystal film. l^u 疋 3 3 film formation is amorphous, and the composition of the film in the film should be more crystallization temperature as described above. The film formation temperature is low, and the composition with less tin content, the lower the crystallization temperature, and the more the amount of tin or antimony, the higher the crystallization temperature, and the water is divided by 1. 〇xl〇-4Pa or more, h 0xl0-】Pa under the conditions of film formation and water: minutes = film formation phase comparison 'crystals of each composition to (10). C or so. Therefore, relative to indium tin (n) x) The composition range of the value of 6.7xl〇), the crystallization temperature at the time of film formation of u&gt;arPa is not up to the shoe, in particular, the film formation condition of the amorphous film is obtained by the partial pressure of L〇x10, above, &quot;xl〇_ipa film formation conditions can be made non-parallel..., for example, crystallizing around the boot: water production: when the partial pressure ratio is lower than h, the above-mentioned crusted -%) =, = effect of the sage, on the other hand, the partial pressure of water is higher than the upper limit (1 · 0 and the time of the knot, the condition of the moon is made amorphous), but the core I is annealed. 2 'The specific resistance (resistivity) of the film is not reduced, and most of the crystallization is poor under the resistance of 5.^ Ω·_. And the molar ratio of 'in relation to indium> Moir + Moer γ 旲 ' with respect to x is not (~2. 9χ1〇Λη(χ)-6. 7χ1(Γ2)

JO 320646 200923973 之值以上範圍時,即便於水之分壓比1. Ox 10 4Pa更低的一 般條件成膜,由於可成膜為結晶化溫度100°C以上的非晶 型膜(參照日本特願2007-095783),並無必要於水之分壓 為1. 0xl0_4Pa以上、1. Oxl(^Pa以下之條件下成膜,但是, 於此等之條件下成膜,無論如何當然可為非晶型膜。 其次,說明闞於本發明中所使用的濺鍍靶之製造方 法,於此僅以範例表示者,製造方法未特別限定該等。 首先,作為構成本發明之濺鍍靶之起始原料,一般而 言為In2〇3、Sn〇2、BaC〇3之粉末,Iri2〇3與BaC〇3預先預锻 燒後成BaIn2〇4,於其中將In2〇3及Sn〇2相混合後使用為佳。 乃係為防止因BaC〇3分解時產生氣體引起氣孔的發生。又, 亦可以該等之單體、化合物、複合氧化物等當作原料,使 用單體、化合物時,務必預先實施透過製成氧化物之步驟。 以所期望之調配率混合該等原料粉末,成形方法未特 別限定,可使用以往眾所周知之各種濕式法或乾式法。 以乾式法而言,可列舉冷壓(Co Id Press)法或熱麗 (Hot Press)法等。冷壓法乃係於成形模中填入混合粉末, 製作成形體,再將其煅燒。熱壓法乃係於成形模内煅燒、 燒結混合粉末。 以濕式法而言,例如,使用過濾式成形法(參照日本特 開平11-286002號公報)為佳。此種過濾式成形法,是由陶 瓷原料漿料減壓排出水分所製得成形體之非水溶性材料所 成的過濾式成形模,具有1個以上之排水孔的成形用下模, 與載置於此成形用下模之上之具有通水性的過濾器,及經由 320646 200923973 •上面側夹住而密封此過濾器之密封材的成形用模框所組 成。上述之成形用下模、成形用模框、密封材及過渡器是各 別可拆解的方式所組m使難從該過濾ϋ同面侧減 [排水水料中的水分之過濾、式成形模,調配由混合粉末、 離子交換水及有機添加劑所成的㈣,將該漿料注入於過 濾式成形模,由該濾網同面側減壓排出漿料中之水分,製 作出成’將製得的喊成形體乾燥創旨後,锻燒。 f 以冷壓法或濕式法成形者的煅燒溫度較佳為1300至 =o°c ’更佳的是刪至165(rc,該環境為大氣環境、 氧氣環境、非氧化性環境或是真空環境等。另-方面,敎 壓法之情況’是於120(rc附近燒結為佳,該環境為非氧化 性環境或真空環境等。又,以各種方法般燒後,實施成形、 加工用之機械加工為規定尺寸而製成靶。 [實施例] 以下乃根據實施例說明本發明,但不以該等為限制。 I (濺鍍靶製造例1至67) 備妥純度&gt; 99.99%之In2〇3粉末、祕粉末,及純度 &gt;99. 9%之 Bac〇3粉末。 首先’以BET=27m/g之in2〇3粉末58. 6重量%及 ΒΕΤ= 1 · 3m2/g之BaC〇3粉末4〗.4重量%之比率,準備合計量 2〇〇g,於乾燥狀態用球磨機混合,在大氣中以㈣。㈢3 小時實施預燒、製得BalmO4粉末。 其次,上述之Ba論粉末、以卿祝/忌之ίη2〇3粉末及 BET=〗. 5mVg之Sn〇2粉末於相對於〗莫耳ίη時,如及如以 320646 12 200923973 ί至表4中所佔之比率’準備大約⑽,以球 二^貝:〜。然後添加入作為黏合劑之PVA水溶液,混合、 冷壓得成形體。在大氣中於赋、ι。小時,每 ◦c:心:ί對:f*形體脫脂’其次,於氧氣環境下於_ 二、凡、日’ ’製得燒結體。具體的梧燒條件是以loot:/h, =升:至80(rc,再以4,c/h’由_。。升溫至献, 小蚪後,以100°C/h之冷卻條件,從160(rc冷卻至室 二丨後加工5亥燒結體製得乾。此時之密度及積體電阻 ’例如在32之組成中,各別是. 咖 22 之組成中’各別是 6. 96g/cm3、2· 87χ1(Γ4Ω . cm。 (試驗實施例A1至A18) 在4英吋之直流磁控濺鐘裝置,各裴設上述各製造例 1至18之濺錢乾,基板溫度為室溫(約2〇。〇),水之分壓為 l_〇xl(T4Pa、_邊變化氧氣分壓於〇至3 〇sccm之間(相當 於0至1. 1x10 2pa),一邊製得試驗實施例A1至A18之透 明導電膜。 濺鍍條件誠如下述,製得厚度為1200 A之膜。 革巴尺寸.0 =4in、t = 6mm。 濺鍍方式:DC磁控濺鍍。 排氣破置·回轉栗(rotary pumpH冷束真空泵(cryo pump)。 到達真空度:5· 3xl(T6[Pa]。When the value of JO 320646 200923973 is more than or equal to the range, the film is formed into a film having a crystallization temperature of 100 ° C or higher, even if the partial pressure of water is less than 1. Ox 10 4Pa. May 2007-095783), it is not necessary to form a film under the conditions of 1. 0xl0_4Pa or more, 1. Oxl (^Pa or less), but film formation under these conditions, of course, may be non- Next, the method for producing a sputtering target used in the present invention will be described, and the production method is not particularly limited. First, as a sputtering target constituting the present invention The starting materials are generally powders of In2〇3, Sn〇2 and BaC〇3, and Iri2〇3 and BaC〇3 are pre-calcined into BaIn2〇4, in which In2〇3 and Sn〇2 are mixed. It is preferable to use it in order to prevent the occurrence of pores due to gas generated when BaC〇3 is decomposed. It is also possible to use such monomers, compounds, composite oxides, etc. as raw materials, and when using monomers or compounds. The step of forming an oxide is carried out in advance. Mixing at a desired blending ratio The raw material powder and the molding method are not particularly limited, and various wet methods or dry methods known in the art can be used. Examples of the dry method include a cold press (Co Id Press) method or a hot press method. The pressing method is to fill a molding powder into a mixed powder to prepare a molded body, which is then calcined. The hot pressing method is to calcine and sinter the mixed powder in a forming mold. In the wet method, for example, a filter forming method is used. The filter molding method is a filter molding method in which a water-insoluble material obtained by decompressing water from a ceramic raw material slurry to obtain a molded body is obtained. a lower mold for forming having one or more drainage holes, a water-permeable filter placed on the lower mold for molding, and a sealing material for sealing the filter through the upper surface of 320646 200923973 The molding die frame is composed of the lower mold for molding, the molding die frame, the sealing material, and the transition piece, which are separately detachable, so that it is difficult to reduce from the same side of the filter raft [drainage material] Moisture filtration The mold is prepared by mixing (4) the mixed powder, the ion-exchanged water and the organic additive, and the slurry is injected into the filter forming mold, and the water in the slurry is discharged under reduced pressure from the same side of the sieve to produce a After the obtained molded body is dried, the calcination temperature is preferably 1300 to = o °c. The better is to delete 165 (rc, the environment) It is an atmospheric environment, an oxygen environment, a non-oxidizing environment, or a vacuum environment. On the other hand, the case of the rolling method is better at 120 (sintering near rc, which is a non-oxidizing environment or a vacuum environment. After being fired in various ways, the machine for forming and machining is machined to a predetermined size to form a target. [Examples] Hereinafter, the present invention will be described based on examples, but not limited thereto. I (sputter target production examples 1 to 67) A purity of &gt; 99.99% of In2〇3 powder, secret powder, and purity &gt; 99.9% of Bac〇3 powder were prepared. First, the total amount of 2 〇〇g of the in2〇3 powder of BET=27m/g is 58.6 wt% and Ba=1 · 3 m2/g of BaC〇3 powder 4 ..4 wt%, and dried. The state is mixed with a ball mill and placed in the atmosphere as (4). (3) Performing calcination in 3 hours to obtain BalmO4 powder. Secondly, the above-mentioned Ba is a powder, and the powder of 祝 祝 忌 忌 忌 及 及 〗 〗 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 The ratio of 'prepared to about (10), to the ball two ^ Bay: ~. Then, a PVA aqueous solution as a binder was added, and the mixture was cold-pressed to obtain a molded body. In the atmosphere, Fu, ι. Hour, every ◦c: heart: ί vs.: f* body degreasing' Secondly, a sintered body is produced in _2, 凡, 日' in an oxygen environment. The specific calcination conditions are: loot: / h, = liter: to 80 (rc, then 4, c / h ' from _.. warmed to the offer, after the small sputum, with 100 ° C / h cooling conditions, From 160 (rc cooling to room two 丨 processing 5 烧结 sintering system to dry. The density and integrated resistance at this time, for example, in the composition of 32, each is. In the composition of the coffee 22 'different is 6. 96g /cm3, 2·87χ1 (Γ4Ω. cm. (Test Examples A1 to A18) In a 4 inch DC magnetron sputtering device, each of the above-described manufacturing examples 1 to 18 is sprinkled with a substrate temperature of room temperature. Temperature (about 2 〇. 〇), the partial pressure of water is l_〇xl (T4Pa, _ side change oxygen partial pressure between 〇 to 3 〇sccm (equivalent to 0 to 1. 1x10 2pa), while making the test The transparent conductive films of Examples A1 to A18. The sputtering conditions were as follows, and a film having a thickness of 1200 A was produced. The size of the grain was .0 = 4 in, t = 6 mm. Sputtering method: DC magnetron sputtering. Broken and rotating chestnut (rotary pumpH cold beam vacuum pump (cryo pump). The degree of vacuum reached: 5 · 3xl (T6 [Pa].

Ar 壓力:4.0xi0-i[Pa]。 氧氣壓力:〇至1. lxl(T2[Pa]。 水壓力:1. 〇xl〇-4[Pa]。 320646 200923973 基板溫度:室溫。 濺鍍電力:130W(電力密度1. 6W/ cm2)。 使用基板:C0RNING#1737(液晶顯示器用玻璃)、t=0. 8mm。 關於試驗實施例A1至A18,求得有關在室溫成膜中之 氧氣分壓與電阻率之關係及於250°C退火後之氧氣分壓與 ' 電阻率之關係。 下述表1中,表示相對於各試樣之1莫耳In,Ba及Sn , 之莫耳比,同時顯示於室溫成膜之結晶狀態(以a表示非晶 型膜、以c表不結晶化膜)’ _員不非晶型艇之結晶化溫度。 表1中成膜時電阻率是於室溫成膜之最佳氧氣分壓中 的膜電阻率。再者,退火後之電阻率是250°C退火時之最 佳氧氣分壓中之電阻率。 再者,表1中顯示之結晶化溫度係如下方式求得。以 250°C退火後於最低電阻率之氧氣分壓,經室溫成膜之膜, 用50°C刻度,由100°C至300°C (必要時500乞)於大氣中進 I: 行1小時之退火,以薄膜xRD分析該膜。關於表示經室溫 成膜之非晶型膜之繞射♦ (ha 1 〇 peak),由於退火溫度變高 被檢測出繞射線。訂定該最初溫度為結晶化溫度。又,結 晶化溫度之其他的求得方法,亦可使用高溫薄膜xRD法。 再者,第1圖中,標繪試驗實施例A1至A18圖形,以 •表示結晶化溫度為100至300°C,以▲表示結晶化溫度 為350°C以上。 由該結果得知,全部試樣之結晶化溫度皆在100°C至 300°C。 14 320646 200923973 [表1] 言劫策 編號 製造 例 &amp;Ί比 Ba比 結晶 狀態 結晶〗bS^(°C) 成膜時電阻率(X 1(ΤΩ . cm) 退火後電阻率(x ΙΟ^Ω · cm) A1 1 0. 05 0.0001 a 150 4.7 3.4 A2 2 0. 05 0.0002 a 150 4.8 3.4 A3 3 0.05 0.0005 a 150 4. 9 3. 5 A4 4 0.05 0.001 a 150 4. 7 3. 6 A5 5 0.05 0.002 a 150 4.7 3.4 A6 6 0.05 0.005 a 150 4.8 3.5 A7 7 0.05 0.01 a 150 5.2 3.6 A8 8 0. 075 0.002 a 150 4.6 2.5 A9 9 0. 075 0.005 a 150 4.8 2.6 A10 10 0.1 0.0001 a 150 4.5 1.9 All 11 0.1 0.0002 a 150 4.5 1.9 A12 12 0.1 0.0005 a 150 4.5 1.9 A13 13 0.1 0.001 a 150 4.5 1.9 A14 14 0.1 0.002 a 150 4.5 1.9 A15 15 0.15 0.0001 a 200 4.7 2.0 A16 16 0. 15 0.0002 a 200 4.7 2.0 A17 17 0.15 0.0005 a 200 4.6 2.0 A18 18 0.2 0.0006 a 250 4.7 2.2 (試驗實施例B1至B18)。 於4英吋之DC磁控濺鍍裝置上各別裝設各製造例1至 18之濺鍍靶,基板溫度為室溫(約20°C),水之分壓為1.0 15 320646 200923973 . xl(T3Pa,一邊變化氧氣分壓於0至3. Osccm之間(相當於0 至1. 1. 0xl0_2Pa),一邊製得試驗實施例Β1至Β18之透明 導電膜。 濺鍍之條件誠如下述,製得厚度為1200 A之膜。 萆巴尺寸:&lt;/&gt; =4in、t=6mm。 濺鍍方式:DC磁控濺鍵。 排氣裝置:回轉泵+冷凍真空泵。 , 到達真空度:5. 3xlO_6[Pa]。Ar pressure: 4.0xi0-i [Pa]. Oxygen pressure: 〇 to 1. lxl (T2 [Pa]. Water pressure: 1. 〇xl〇-4 [Pa]. 320646 200923973 substrate temperature: room temperature. Sputtering power: 130W (power density 1. 6W / cm2) The substrate was used: C0RNING #1737 (glass for liquid crystal display), t=0. 8 mm. With respect to Test Examples A1 to A18, the relationship between the oxygen partial pressure and the resistivity in film formation at room temperature was obtained at 250°. The relationship between the partial pressure of oxygen after C annealing and the resistivity. Table 1 below shows the molar ratio of 1 mol of In, Ba and Sn relative to each sample, and shows the crystal formation at room temperature. State (a indicates amorphous film, c indicates non-crystallized film) ' _ non-amorphous boat crystallization temperature. Table 1 in the film formation resistivity is the best oxygen content at room temperature film formation The film resistivity in the press. Further, the resistivity after annealing is the resistivity in the optimum oxygen partial pressure at the annealing of 250 ° C. Further, the crystallization temperature shown in Table 1 is obtained as follows. After annealing at 250 °C, the partial pressure of oxygen at the lowest resistivity, film formed at room temperature, at 50 ° C, from 100 ° C to 300 ° C (500 必要 if necessary) to the atmosphere I: Annealing for 1 hour, the film was analyzed by film xRD. Regarding the diffraction ♦ (ha 1 〇peak) of the amorphous film formed at room temperature, the ray was detected because the annealing temperature became high. The initial temperature is determined as the crystallization temperature. Further, the other method for determining the crystallization temperature may be a high temperature film xRD method. Further, in Fig. 1, the test examples A1 to A18 are plotted to • The crystallization temperature is 100 to 300 ° C, and the crystallization temperature is 350 ° C or higher. From the results, the crystallization temperatures of all the samples are 100 ° C to 300 ° C. 14 320646 200923973 [ Table 1] Snapshot numbering manufacturing example &amp; ratio Ba ratio crystal state crystallization bS^(°C) resistivity at film formation (X 1 (ΤΩ. cm) resistivity after annealing (x ΙΟ^Ω · cm) A1 1 0. 05 0.0001 a 150 4.7 3.4 A2 2 0. 05 0.0002 a 150 4.8 3.4 A3 3 0.05 0.0005 a 150 4. 9 3. 5 A4 4 0.05 0.001 a 150 4. 7 3. 6 A5 5 0.05 0.002 a 150 4.7 3.4 A6 6 0.05 0.005 a 150 4.8 3.5 A7 7 0.05 0.01 a 150 5.2 3.6 A8 8 0. 075 0.002 a 150 4.6 2.5 A9 9 0. 075 0.005 a 150 4.8 2.6 A10 10 0.1 0.0001 a 150 4.5 1.9 All 11 0.1 0.0002 a 150 4.5 1.9 A12 12 0.1 0.0005 a 150 4.5 1.9 A13 13 0.1 0.001 a 150 4.5 1.9 A14 14 0.1 0.002 a 150 4.5 1.9 A15 15 0.15 0.0001 a 200 4.7 2.0 A16 16 0. 15 0.0002 a 200 4.7 2.0 A17 17 0.15 0.0005 a 200 4.6 2.0 A18 18 0.2 0.0006 a 250 4.7 2.2 (Test Examples B1 to B18). The sputtering targets of each of the manufacturing examples 1 to 18 were separately mounted on a 4 inch DC magnetron sputtering apparatus, the substrate temperature was room temperature (about 20 ° C), and the partial pressure of water was 1.0 15 320646 200923973 . xl (T3Pa, a transparent conductive film of Test Examples Β1 to Β18 was prepared while varying the oxygen partial pressure between 0 and 3. Osccm (corresponding to 0 to 1.1.0xx0_2Pa). The conditions of the sputtering were as follows. A film having a thickness of 1200 A is produced. The size of the bar: &lt;/&gt; = 4 in, t = 6 mm. Sputtering method: DC magnetron splash button. Exhaust device: rotary pump + refrigerated vacuum pump. , reaching vacuum: 5. 3xlO_6[Pa].

Ar 壓力:4· OxlO_I[Pa]。 氧氣壓力:0至1. lxl(T2[Pa]。 水壓力:1.0xl03[Pa]。 基板溫度:室溫。 濺鍍電力:130W(電力密度1. 6W/ cm2)。 使用基板:C0RNING#1737(液晶顯示器用玻璃)、t=0. 8mra 關於試驗實施例B1至B18,求得室溫成膜之氧氣分壓 k 與電阻率之關係及以250°C退火後之氧氣分壓與電阻率之 關係。 下述之表2中,表示相對於各試樣之1莫耳In時,Ba 及Sn之莫耳比,顯示於室溫成膜之結晶狀態(以a當作非 晶型膜、以c當作結晶化膜)之同時亦顯示非晶型膜之結晶 化溫度。又,結晶化溫度、成膜時電阻率、退火後電阻率 誠如上述者。 再者,於第2圖中標記試驗實施例B1至B18,以#表 示結晶化溫度為100至300°C,以▲表示結晶化溫度為350 16 320646 200923973 . °c以上。 結果得知,關於全部試樣之結晶化溫度為100°C至300°C。 [表2] 試樣 編號 製造 例 Sn比 Ba比 結晶 狀態 結晶化溫 度rc) 成膜時電阻率 (χΙΟ^Ω · cm) 退火後電阻率 (χΙΟ^Ω cm) B1 1 0. 05 0.0001 a 200 4.7 3.5 B2 2 0.05 0.0002 a 200 4.8 3.5 B3 3 0.05 0.0005 a 200 4.9 3.5 B4 4 0.05 0.001 a 200 4.9 3.4 B5 5 0. 05 0.002 a 200 4.9 3.5 B6 6 0. 05 0.005 a 200 5.0 3.6 B7 7 0.05 0.01 a 200 5.4 3.6 B8 8 0.075 0.002 a 200 4.8 2.6 B9 9 0.075 0.005 a 200 4.9 2.7 B10 10 0.1 0.0001 a 200 4.5 2.1 B11 11 0.1 0.0002 a 200 4.5 2.0 B12 12 0.1 0.0005 a 200 4.6 2.1 B13 13 0.1 0.001 a 200 4.6 2.1 B14 14 0.1 0.002 a 200 4.7 2.1 B15 15 0.15 0.0001 a 250 4.6 2.2 B16 16 0.15 0.0002 a 250 4.7 2. 0 B17 17 0.15 0.0005 a 250 4.7 2.2 B18 18 0.2 0. 0006 a 300 4.9 2.4 17 320646 200923973 . (參考試驗例Cl至C67)。 於4英吋之DC磁控濺鍍裝置上各別裝設各製造例1至67 之濺鍍靶,基板溫度為室溫(約20°C),水之分壓為1.Ox 10—5Pa,一邊變化氧氣分壓於0至3. Osccm之間(相當於0至 1. 1. 0xl0_2Pa),一編製得參考試驗例C1至C67之透明導電膜。 — 濺鍍之條件誠如下述,製得厚度為1200 A之膜。 革巴尺寸:0 =4in、t=6mm 〇 , 濺鍍方式:DC磁控濺鍍。 排氣裝置:回轉泵+冷凍真空泵。 到達真空度:5. 3xlO_6[Pa]。Ar pressure: 4 · OxlO_I [Pa]. Oxygen pressure: 0 to 1. lxl (T2 [Pa]. Water pressure: 1.0xl03 [Pa]. Substrate temperature: room temperature. Sputtering power: 130 W (power density 1. 6 W/cm2). Substrate: C0RNING #1737 (glass for liquid crystal display), t=0. 8mra For the test examples B1 to B18, the relationship between the oxygen partial pressure k at room temperature and the resistivity and the oxygen partial pressure and resistivity after annealing at 250 ° C were obtained. In the following Table 2, the molar ratio of Ba and Sn in the case of 1 mol of In for each sample is shown in a crystalline state at room temperature (a is regarded as an amorphous film, When c is used as the crystallization film), the crystallization temperature of the amorphous film is also exhibited. Further, the crystallization temperature, the resistivity at the time of film formation, and the resistivity after annealing are as described above. Further, in Fig. 2 The test examples B1 to B18 were marked with a crystallization temperature of 100 to 300 ° C and a crystallization temperature of 350 16 320646 200923973 ° ° C with ▲. As a result, it was found that the crystallization temperature of all the samples was 100 ° C to 300 ° C. [Table 2] Sample No. Production Example Sn Ratio of Ba to Crystallization State Crystallization Temperature rc) Resistivity at Film Formation (χΙΟ^Ω · cm) Resistivity after annealing (χΙΟ^Ω cm) B1 1 0. 05 0.0001 a 200 4.7 3.5 B2 2 0.05 0.0002 a 200 4.8 3.5 B3 3 0.05 0.0005 a 200 4.9 3.5 B4 4 0.05 0.001 a 200 4.9 3.4 B5 5 0. 05 0.002 a 200 4.9 3.5 B6 6 0. 05 0.005 a 200 5.0 3.6 B7 7 0.05 0.01 a 200 5.4 3.6 B8 8 0.075 0.002 a 200 4.8 2.6 B9 9 0.075 0.005 a 200 4.9 2.7 B10 10 0.1 0.0001 a 200 4.5 2.1 B11 11 0.1 0.0002 a 200 4.5 2.0 B12 12 0.1 0.0005 a 200 4.6 2.1 B13 13 0.1 0.001 a 200 4.6 2.1 B14 14 0.1 0.002 a 200 4.7 2.1 B15 15 0.15 0.0001 a 250 4.6 2.2 B16 16 0.15 0.0002 a 250 4.7 2. 0 B17 17 0.15 0.0005 a 250 4.7 2.2 B18 18 0.2 0. 0006 a 300 4.9 2.4 17 320646 200923973 . (Reference test examples Cl to C67). The sputtering targets of each of the manufacturing examples 1 to 67 are respectively mounted on a 4 inch DC magnetron sputtering apparatus, the substrate temperature is room temperature (about 20 ° C), and the partial pressure of water is 1.Ox 10 - 5 Pa. While changing the oxygen partial pressure between 0 and 3. Osccm (equivalent to 0 to 1. 1. 0xl0_2Pa), a transparent conductive film of Reference Examples C1 to C67 was prepared. — The conditions of the sputtering are as follows, and a film having a thickness of 1200 A is obtained. Geba size: 0 = 4in, t = 6mm 〇, sputtering method: DC magnetron sputtering. Exhaust device: rotary pump + refrigerated vacuum pump. The degree of vacuum reached: 5. 3xlO_6 [Pa].

Ar 壓力:4. Oxl(r][Pa]。 氧氣壓力:0至1. lxl(T2[Pa]。 水壓力:1. 0xl(T5[Pa]。 基板溫度:室溫。 濺鍍電力:130W(電力密度1. 6W/cm2)。 ,使用基板:C0RNING#1737(液晶顯示器用玻璃)、t=0. 8mm 關於參考試驗例Cl至C67,求得於室溫成膜中之氧氣 分壓與電阻率之關係及於250°C退火後之氧氣分壓與電阻 率之關係。 下述表3及表4中,是表示相對於各試樣之1莫耳In 時’ Ba.及Sn之莫耳比’顯不於室溫成膜之結晶狀態(以a 當作非晶型膜、以c當作結晶化膜)之同時亦顯示非晶型膜 之結晶化溫度。再者’結晶化溫度、成膜時電阻率、退火 後電阻率誠如上述者。 18 320646 200923973 =2造例乾,求得在室溫(約肌) 长分壓下,成膜後之膜的電阻率之闞係, 水付取佳虱矾分壓之同瞎,由 〆 t . 各虱虱y刀壓成膜之膜,於250 C,火後之祿率與成膜氧氣分壓之關係,以退 :且^最低電阻的氧氣分廢作為於啊成膜時之最佳氧 =壓’:斷兩者之間之最佳氧氣分星 圖中,以籲表示不同,以▲表示幾乎相同。 銦科對於銦1料之錫的莫料y,相對於 1〇’之伯、·貝的莫耳比以X表示為(~2.9xl(T2Ln〇〇-6.7x )之值以上、在(_2 nun-iT ,、 了 v=〇n 士 η(Χ)—4·6Χ10,之值以下,除 $八段命^ ’朗後之非晶型卿成低f阻之成膜氧 ::塗得=後2Γ臈繼電阻之成膜氧氣分壓不相同, 分壓不才1同。亦^之最佳氧氣分壓與在室溫之最佳氧氣 之低電阻i在該等組成範圍’並非由成膜後當時 化膜以刑成:Γ取佳氧氣分壓’較佳者是退火後之經結晶 阻;變:=阻之氧氣分壓成膜後,退火後之膜的電 J 4 /于去相對於姻1莫耳之錫的莫耳比y,相對於銦 料邮X絲絲達(_2. 9航心)-6. 7x 、乾圍日守,結晶溫度是比loot小的範圍。 八 #如第1圖及第2圖所表示者,得知將水之 S於銦膜時’相對於銦1莫耳之錫的莫耳比y, 10-W W 7 的莫耳比以X表示為未達(―2.9x • xl〇 )之值的範圍時,結晶溫度便高為150。〇 320646 19 200923973 , 以上,易成膜為非晶型膜。 [表3] 試樣 編號 製造 例 Sn比 Ba比 結晶 狀態 結晶化溫 度rc) 成膜時電阻率(X 1(ΤΩ · cm) 退火後電阻率 (χ10'4Ω · cm) C19 19 0 0.1 a &gt;450 19.2 21.4 C20 20 0.025 0.07 a 400 12.7 14.3 C21 21 0.025 0.1 a &gt;450 15.3 17.5 C1 1 0.05 0.0001 c &lt;100 4. 6 3.3 C2 2 0.05 0.0002 c &lt;100 4. 7 3.4 C3 3 0. 05 0. 0005 c &lt;100 4.8 3.4 C4 4 0. 05 0. 001 c &lt;100 4. 7 3.5 C5 5 0.05 0.002 c &lt;100 4. 2 3.0 C6 6 0.05 0.005 c &lt;100 4.2 3.1 C7 7 0.05 0. 01 c &lt;100 4.3 3.4 C22 22 0.05 0. 02 a 150 5.2 4.9 C23 23 0.05 0. 03 a 200 7.5 6.2 C24 24 0.05 0. 05 a 400 8.2 9.2 C8 8 0.075 0. 002 c &lt;100 3.3 2.1 C9 9 0.075 0.005 c &lt;100 3.4 2.1 C25 25 0.075 0. 01 a 100 4.2 3. 1 C26 26 0.075 0. 02 a 150 5.1 3.5 C27 27 0. 075 0. 03 a 250 6.7 5. 1 C10 10 0.1 0. 0001 c &lt;100 4.4 1.8 C11 11 0.1 0.0002 c &lt;100 4.4 1.8 20 320646 200923973 C12 12 0.1 0.0005 C &lt;100 4.4 1.8 Γ13 13 0.1 0.001 c &lt;100 4.4 1.8 C14 14 0.1 0.002 c &lt;100 4.5 1.8 C28 28 0.1 0.005 a 100 4. 5 1.8 C29 29 0.1 0.01 a 150 4. 7 2.3 C30 30 0.1 0.02 a 200 5. 6 2.7 C31 31 0.1 0.03 a 250 6. 1 4. 6 C32 32 0.1 0.05 a 400 8. 6 10.0 C33 33 0.1 0.1 a &gt;450 14.2 15.3 C15 15 0.15 0.0001 c &lt;100 4. 7 1.8 C16 16 0.15 0.0002 c &lt;100 4. 7 1.8 C17 17 0.15 0.0005 c &lt;100 4. 8 1.8 C34 34 0.15 0.001 a 150 4. 6 1.8 C35 35 0.15 0.002 a 150 4. 6 .1.8 C36 36 0.15 0. 005 a 150 4.8 1.8 ί. 21 320646 200923973 ,[表 4] 試樣 編號 製造 例 Sn比 Ba比 結晶 狀態 結晶化溫 度rc) 成膜時電阻率 (χ10&quot;4Ω · cm) 退火後電阻率 (χ10'4Ω · cm) C37 37 0.15 0.01 a 200 5. 0 2.1 C38 38 0. 15 0.02 a 250 6.0 2.6 C30 30 0. 15 0.03 a 350 7. 0 5.9 C40 40 0.15 0. 05 a &gt;450 8.6 8.1 C18 18 0.2 0.00006 a &lt;100 4.9 1.9 C41 41 0.2 0.0001 a 150 4.8 1.9 C42 42 0.2 0.0002 a 150 4.8 1.9 C43 43 0.2 0.0005 a 150 4. 8 1.9 C44 44 0.2 0.001 a 200 4.8 1.9 C45 45 0.2 0.002 a 200 4. 9 1.9 C46 46 0.2 0.005 a 200 5. 2 1.9 C47 47 0.2 0.01 a 200 5. 9 2.4 C48 48 0.2 0.02 a 250 6. 7 3. 0 C49 49 0.2 0. 03 a 400 8. 0 6.2 C50 50 0.2 0.05 a &gt;450 10.3 9.8 C51 51 0.22 0. 00005 a 100 4. 9 2.0 C52 52 0.22 0. 033 a 400 8. 1 6.3 C53 53 0.25 0. 0001 a 250 4. 7 2.1 C54 54 0. 25 0.0002 a 250 4. 7 2.1 C55 55 0.25 0.0005 a 250 4. 7 2.1 22 320646 200923973Ar pressure: 4. Oxl (r) [Pa]. Oxygen pressure: 0 to 1. lxl (T2 [Pa]. Water pressure: 1. 0xl (T5 [Pa]. Substrate temperature: room temperature. Sputtering power: 130W (Power density: 1.6 W/cm2). Substrate used: C0RNING #1737 (glass for liquid crystal display), t=0. 8 mm For reference test examples C1 to C67, the oxygen partial pressure in the film formation at room temperature was determined. The relationship between the resistivity and the partial pressure of oxygen after annealing at 250 ° C. The following Tables 3 and 4 show the difference between Ba and Sn for 1 mol of In with respect to each sample. The ear ratio is not crystallized at room temperature (a is used as an amorphous film and c is used as a crystallized film), and the crystallization temperature of the amorphous film is also exhibited. The resistivity at the time of film formation and the resistivity after annealing are as described above. 18 320646 200923973 = 2 The dry form is obtained, and the resistivity of the film after film formation is obtained at room temperature (about muscle) long partial pressure. The water is paid by the same pressure, and the pressure is determined by the relationship between ^Minimum resistance of oxygen Waste as the best oxygen in the film formation = pressure ': the best oxygen star between the two, the difference between the two, to call the difference, to ▲ is almost the same. Indium Branch for the indium 1 tin The material y is expressed by X as the value of (~2.9xl(T2Ln〇〇-6.7x) with respect to 1伯', and (_2 nun-iT , , v=〇n士(Χ)—4·6Χ10, the value below, except for the eight-segment life ^ 'After-formed amorphous type Qingcheng low f resistance filming oxygen:: coating = after 2 Γ臈 subsequent resistance filming Oxygen partial pressure is not the same, partial pressure is not the same. Also ^ the best oxygen partial pressure and the lowest oxygen resistance at room temperature i in the composition range 'is not formed by the film at the time of film formation : Γ 佳 good oxygen partial pressure 'better is the crystallization resistance after annealing; change: = resist oxygen partial pressure film formation, after annealing the film of electricity J 4 / to go relative to the marriage 1 Mo tin Mohby y, relative to the indium material, the mail X wire (_2. 9 navigation) - 6. 7x, dry day, the crystallization temperature is smaller than the loot range. Eight # as the first picture and the second As shown in the figure, it is known that when the S of water is in the indium film, it is relative to the tin of indium 1 When the molar ratio of Mobi y, 10-WW 7 is expressed as X in the range of less than (-2.9x • xl〇), the crystallization temperature is as high as 150. 〇320646 19 200923973, above, easy film formation It is an amorphous film. [Table 3] Sample No. Production Example Sn Ratio of Ba to Crystallization State Crystallization Temperature rc) Resistivity at Film Formation (X 1 (ΤΩ · cm) Resistivity after Annealing (χ10'4Ω · cm) C19 19 0 0.1 a &gt; 450 19.2 21.4 C20 20 0.025 0.07 a 400 12.7 14.3 C21 21 0.025 0.1 a &gt;450 15.3 17.5 C1 1 0.05 0.0001 c &lt;100 4. 6 3.3 C2 2 0.05 0.0002 c &lt;100 4. 7 3.4 C3 3 0. 05 0. 0005 c &lt;100 4.8 3.4 C4 4 0. 05 0. 001 c &lt;100 4. 7 3.5 C5 5 0.05 0.002 c &lt;100 4. 2 3.0 C6 6 0.05 0.005 c &lt 100 4.2 3.1 C7 7 0.05 0. 01 c &lt; 100 4.3 3.4 C22 22 0.05 0. 02 a 150 5.2 4.9 C23 23 0.05 0. 03 a 200 7.5 6.2 C24 24 0.05 0. 05 a 400 8.2 9.2 C8 8 0.075 0 002 c &lt;100 3.3 2.1 C9 9 0.075 0.005 c &lt;100 3.4 2.1 C25 25 0.075 0. 01 a 100 4.2 3. 1 C26 26 0.075 0. 02 a 150 5.1 3.5 C27 27 0. 075 0. 03 a 250 6.7 5. 1 C10 10 0.1 0. 0001 c &lt;100 4.4 1.8 C11 11 0.1 0.0002 c &lt;100 4.4 1.8 20 320646 200923973 C12 12 0.1 0.0005 C &lt;100 4.4 1.8 Γ13 13 0.1 0.001 c &lt;100 4.4 1.8 C14 14 0.1 0.002 c &lt;100 4.5 1.8 C28 28 0.1 0.005 a 100 4. 5 1.8 C29 29 0.1 0.01 a 150 4. 7 2.3 C30 30 0.1 0.02 a 200 5. 6 2.7 C31 31 0.1 0.03 a 250 6. 1 4. 6 C32 32 0.1 0.05 a 400 8. 6 10.0 C33 33 0.1 0.1 a &gt;450 14.2 15.3 C15 15 0.15 0.0001 c &lt;100 4. 7 1.8 C16 16 0.15 0.0002 c &lt;100 4. 7 1.8 C17 17 0.15 0.0005 c &lt;100 4. 8 1.8 C34 34 0.15 0.001 a 150 4. 6 1.8 C35 35 0.15 0.002 a 150 4. 6 .1.8 C36 36 0.15 0. 005 a 150 4.8 1.8 ί. 21 320646 200923973 , [Table 4] Sample No. Manufacturing Example Sn is crystallized in a crystal state than Ba Temperature rc) Resistivity at film formation (χ10&quot;4Ω · cm) Resistivity after annealing (χ10'4Ω · cm) C37 37 0.15 0.01 a 200 5. 0 2.1 C38 38 0. 15 0.02 a 250 6.0 2.6 C30 30 0. 15 0.03 a 350 7. 0 5.9 C40 40 0.15 0. 05 a &gt;450 8.6 8.1 C18 18 0.2 0.00006 a &lt;100 4.9 1.9 C41 41 0.2 0.0001 a 150 4.8 1.9 C42 42 0.2 0.0002 a 150 4.8 1.9 C43 43 0.2 0.0005 a 150 4. 8 1.9 C44 44 0.2 0.001 a 200 4.8 1.9 C45 45 0.2 0.002 a 200 4. 9 1.9 C46 46 0.2 0.005 a 200 5. 2 1.9 C47 47 0.2 0.01 a 200 5. 9 2.4 C48 48 0.2 0.02 a 250 6. 7 3. 0 C49 49 0.2 0. 03 a 400 8. 0 6.2 C50 50 0.2 0.05 a &gt;450 10.3 9.8 C51 51 0.22 0. 00005 a 100 4. 9 2.0 C52 52 0.22 0. 033 a 400 8. 1 6.3 C53 53 0.25 0. 0001 a 250 4. 7 2.1 C54 54 0. 25 0.0002 a 250 4. 7 2.1 C55 55 0.25 0.0005 a 250 4. 7 2.1 22 320646 200923973

(試驗實施例A68至A73)。 得由下述表 中 V.. 與職鏡乾製造例1至67相同方式,製计田下述 所表示的組成之燒結體所成的製造例⑽至乃之靶。 於4英忖之DC磁控賤鍍裝置上各別裝設各製巴造例卟 基板溫度為室溫(約抓),水之分麗為 二Pa,一邊變化氧氣分壓為〇至3.〇SCCm之間(相當 0至卜1.0x10 Pa) ’ -邊製得試驗實施例A68至A73 之透明導電膜。 濺錄之條件誠如下述,製得厚度為麗a之膜。 革巴尺寸.0 =4in、t=6mm。 濺鍍方式:DC磁控濺鍍。 23 320646 200923973 , 排氣裝置:回轉泵+冷凍真空泵。 到達真空度:5. 3xlO_6[Pa]。(Test Examples A68 to A73). The production example (10) to the target of the sintered body having the composition shown below is prepared in the same manner as in the following Tables V.. On the 4 inch DC magnetron plating device, each board is equipped with a temperature of room temperature (about scratch), the water is divided into two Pa, and the oxygen partial pressure is changed to 3. A transparent conductive film of Test Examples A68 to A73 was prepared between 〇SCCm (corresponding to 0 to 1.0x10 Pa). The conditions for the splattering are as follows, and a film having a thickness of 丽a is obtained. Geba size. 0 = 4in, t = 6mm. Sputtering method: DC magnetron sputtering. 23 320646 200923973 , Exhaust device: rotary pump + refrigerated vacuum pump. The degree of vacuum reached: 5. 3xlO_6 [Pa].

Ar 壓力:4. OxliT1 [Pa]。 氧氣壓力:0至1. 1x10—2[Pa]。 水壓力:1. 0xl0_4[Pa]。 基板溫度:室溫。 濺鍍電力:130W(電力密度1. 6W/ cm2)。 使用基板:C0RNING#1737(液晶顯示器用玻璃)、t=0.8mm 關於試驗實施例A68至A73,求得室溫成膜時之氧氣 分壓與電阻率之關係及以250°C之退火後的氧氣分壓與電 阻率之關係。 下述之表5中,表示相對於各態樣之銦1莫耳時,Ba 及Sn之莫耳比,顯示室溫成膜之結晶狀態(以a當作非晶 型膜、以c當作結晶化膜)之同時,亦顯示非晶型膜之結晶 化溫度。再者,結晶化溫度、成膜時電阻率、退火後電阻 , 率誠如上述者。 再者,在第1圖1中,將試驗實施例A68至A73與試 驗實施例A1至A18 —起標記繪圖,以鲁表示結晶化溫度為 100至300°C,以▲表示結晶化溫度為350°C以上。 結果,得知關於全部試樣之結晶化溫度為100°C至300 24 320646 200923973 .[表 5] 式樣 編號 製造 例 Sn比 Ba比 結晶 狀態 結晶化溫 度rc) 成膜時電阻率 (χ10'4Ω · cm) 退火後電阻率 (χΙΟ^Ω · cm) A68 68 0.025 0.00005 a 100 5.6 4.2 A69 69 0.025 0.001 a 100 5. 7 4.3 A70 70 0.025 0.01 a 200 6.2 4. 9 A71 71 0.05 0.00001 a 150 4. 7 3.3 A72 72 0.15 0.00002 a 200 4.6 2 A73 73 0.2 0.00001 a 250 4.6 2.2 (試驗貫施例B 6 8至B 7 3)。 於4英吋之DC磁控濺鍍裝置上各別裝設各製造例68 至73之濺鍍靶,基板溫度為室溫(約20°C),水之分壓為 1.0xl0—3Pa,一邊變化氧氣分壓為0至3.0sccm之間(相當 於0至1. lxl(T2Pa),一邊製得試驗實施例B68至B73之透 I 明導電膜。 濺鍍之條件係與試驗實施例A68至A73相同,製得厚 度為1200 A之膜。 關於試驗貫施例B 6 8至B 7 3 ’求得在室溫成版之氣氣 分壓與電阻率之關係及以250°C之退火後之氧氣分壓與電 阻率之關係。 下述之表6中,乃係表示相對於各試樣之1莫耳In 時,Ba及Sn之莫耳比,顯示室溫成膜之結晶狀態(以a當 作非晶型膜、以c當作結晶化膜)之同時,亦顯示非晶型膜 25 320646 200923973 r 之結晶化溫度。再者’結晶化溫度、成膜時電阻率、退火 後電阻率誠如上述者。 再者,在第2圖中,將試驗實施例B68至B73與試驗 實施例B1至B18 —起標記,以•表示結晶化溫度為100至 300°C,以▲表示結晶化溫度為350°C以上。 結果,得知關於全部試樣之結晶化溫度為100°C至300 °C。 [表6] 試樣 編號 製造 例 Sn比 Ba比 結晶 狀態 結晶化溫 度(°C) 成膜時電阻率 (χ10'4Ω · cm) 退火後電阻率 (χ10'4Ω · cm) B68 68 0.025 0.00005 a 150 5.7 4.4 B69 69 0.025 0. 001 a 150 5. 9 4.4 B70 70 0.025 0.02 a 250 6.3 5.0 B71 71 0. 05 0.00001 a 200 4. 7 3.5 B72 72 0.15 0.00002 a 250 4. 5 2.1 B73 73 0.2 0.00001 a 300 4. 9 2.4 (參考試驗例C68至C73)。 於4英吋之DC磁控濺鍍裝置上各別裝設各製造例68 至73之濺鍍靶,基板溫度為室溫(約20°C),水之分壓為 1. 0x1 (PPa,一邊變化氧氣分壓為0至3. 0seem之間(相當 於0至1. lxl(T2Pa),一邊製得參考試驗例C68至C73之透 明導電膜。 濺鍍之條件,係與試驗實施例A68至A73相同,製得 26 320646 200923973 . 厚度為1200 A之膜。 關於參考試驗例C68至C73,求得在室溫成膜之氧氣 分壓與電阻率之關係及以250°C退火後之氧氣分壓與電阻 率之關係。 下述表7中,乃係表示相對於各試樣之1莫耳In時, ’ Ba及Sn之莫耳比,顯示室溫成膜之結晶狀態(以a當作非 晶型膜、以c當作結晶化膜)之同時,亦顯示非晶型膜之結 f 晶化溫度。再者,結晶化溫度、成膜時電阻率、退火後電 阻率皆誠如上述者。 再者,在第3圖中,將試驗實施例C68至C73之結果 與參考試驗例C1至C67 —起標記圖形,亦即,關於製造例 68至73之靶,求得在室溫(約20°C)之氧氣分壓與在該分 壓下成膜之膜的電阻率之關係後,求出最佳氧氣分壓同 時,由各氧氣分壓成膜之膜,於250°C退火後之電阻率與 成膜氧氣分壓之關係,由退火後之電阻率為最低電阻之氧 〔 氣分壓當作在250°C成膜之時的最佳氧氣分壓,判斷兩者 之最佳氧氣分壓是否不同,第3圖中以#表示不同者,以 ▲表示幾乎相同者。 27 320646 200923973 [表7]Ar pressure: 4. OxliT1 [Pa]. Oxygen pressure: 0 to 1. 1x10-2 [Pa]. Water pressure: 1. 0xl0_4 [Pa]. Substrate temperature: room temperature. Sputtering power: 130W (power density 1. 6W / cm2). Substrate used: C0RNING #1737 (glass for liquid crystal display), t = 0.8 mm With respect to Test Examples A68 to A73, the relationship between the oxygen partial pressure and the specific resistance at room temperature film formation and annealing at 250 ° C were obtained. The relationship between oxygen partial pressure and resistivity. Table 5 below shows the molar ratio of Ba and Sn with respect to the indium 1 mol of each aspect, and shows the crystalline state of film formation at room temperature (a is regarded as an amorphous film, and c is regarded as At the same time as the crystallized film), the crystallization temperature of the amorphous film is also shown. Further, the crystallization temperature, the resistivity at the time of film formation, and the resistance after annealing are as described above. Further, in Fig. 1, test examples A68 to A73 are labeled with test examples A1 to A18, and the crystallization temperature is 100 to 300 ° C, and the crystallization temperature is 350 by ▲. Above °C. As a result, it was found that the crystallization temperature for all the samples was 100 ° C to 300 24 320646 200923973. [Table 5] Model number Manufacturing example Sn ratio Ba ratio crystal state crystallization temperature rc) Resistivity at the time of film formation (χ10'4 Ω · cm) Resistivity after annealing (χΙΟ^Ω · cm) A68 68 0.025 0.00005 a 100 5.6 4.2 A69 69 0.025 0.001 a 100 5. 7 4.3 A70 70 0.025 0.01 a 200 6.2 4. 9 A71 71 0.05 0.00001 a 150 4. 7 3.3 A72 72 0.15 0.00002 a 200 4.6 2 A73 73 0.2 0.00001 a 250 4.6 2.2 (Test Example B 6 8 to B 7 3). The sputtering targets of each of the manufacturing examples 68 to 73 were separately mounted on a 4 inch DC magnetron sputtering apparatus. The substrate temperature was room temperature (about 20 ° C), and the partial pressure of water was 1.0 x 10 -3 Pa. The varying oxygen partial pressure was between 0 and 3.0 sccm (corresponding to 0 to 1. lxl (T2Pa), and the transparent conductive films of Test Examples B68 to B73 were prepared. The conditions of the sputtering were the same as in Test Example A68. A73 was the same, and a film having a thickness of 1200 A was obtained. About the test Example B 6 8 to B 7 3 'The gas partial pressure and resistivity at room temperature were determined and after annealing at 250 ° C The relationship between the partial pressure of oxygen and the specific resistance. Table 6 below shows the molar ratio of Ba and Sn with respect to 1 mol of In for each sample, showing the crystalline state of film formation at room temperature (in terms of a is used as an amorphous film and c is used as a crystallization film), and the crystallization temperature of the amorphous film 25 320646 200923973 r is also shown. Further, 'crystallization temperature, resistivity at film formation, and resistance after annealing In the second figure, Test Examples B68 to B73 are labeled with Test Examples B1 to B18, and the crystallization temperature is 1. 00 to 300 ° C, ▲ indicates that the crystallization temperature is 350 ° C or higher. As a result, it is found that the crystallization temperature of all the samples is from 100 ° C to 300 ° C. [Table 6] Sample No. Manufacturing Example Sn ratio Ba ratio Crystallization crystallization temperature (°C) Resistivity at film formation (χ10'4Ω · cm) Resistivity after annealing (χ10'4Ω · cm) B68 68 0.025 0.00005 a 150 5.7 4.4 B69 69 0.025 0. 001 a 150 5. 9 4.4 B70 70 0.025 0.02 a 250 6.3 5.0 B71 71 0. 05 0.00001 a 200 4. 7 3.5 B72 72 0.15 0.00002 a 250 4. 5 2.1 B73 73 0.2 0.00001 a 300 4. 9 2.4 (Refer to Test Case C68 to Cx) The sputtering target of each of the manufacturing examples 68 to 73 is mounted on a 4 inch DC magnetron sputtering device, the substrate temperature is room temperature (about 20 ° C), and the partial pressure of water is 1. 0x1 (PPa, while changing the partial pressure of oxygen to 0 to 3. 0seem (equivalent to 0 to 1. lxl (T2Pa), while preparing the transparent conductive film of reference test examples C68 to C73. Conditions of sputtering, system and test In the same manner as in Examples A68 to A73, a film having a thickness of 1200 A was obtained. With respect to Reference Test Examples C68 to C73, the partial pressure of oxygen formed at room temperature was determined. Relationship between the resistivity and oxygen at 250 ° C annealing after the partial pressure with the resistivity. In the following Table 7, the molar ratio of 'B and Sn' with respect to 1 mol of In for each sample shows the crystal state of film formation at room temperature (a is regarded as an amorphous film, and c is used. As the crystallized film, the crystal crystallization temperature of the amorphous film is also shown. Further, the crystallization temperature, the resistivity at the time of film formation, and the resistivity after annealing are all as described above. Further, in Fig. 3, the results of Test Examples C68 to C73 were marked with reference to Test Examples C1 to C67, that is, with respect to the targets of Production Examples 68 to 73, at room temperature (about 20 °C) The relationship between the oxygen partial pressure and the resistivity of the film formed under the partial pressure, and then the optimum oxygen partial pressure is obtained, and the film formed by partial pressure of each oxygen is annealed at 250 ° C. The relationship between the resistivity and the partial pressure of the film forming oxygen, the resistivity after annealing is the lowest resistance of oxygen [gas partial pressure is taken as the optimum oxygen partial pressure at the time of film formation at 250 ° C, and the best oxygen for both is judged. Whether the partial pressure is different, in Fig. 3, # indicates different, and ▲ indicates almost the same. 27 320646 200923973 [Table 7]

(確認氫存在之實驗)。 於4英吋之DC磁控減:鑛裝置上各別裝設製造例13之 濺鍍靶,基板溫度為室溫(約2〇。〇,水之分壓為〗.〇&gt;&lt; M/a(當作實施例丨)、5· 〇xl〇-3pa(當作實施例幻及&amp; 〇χ 10 Pa(當作比較例丨)之3項條件,製得實施例丨、實施例 2及比較例1之透明導電膜。 濺鍍之條件誠如下述,製得厚度為1200 A之膜。 ΐ巴尺寸.0 =4in、t=6mm。 賤鑛方式:DC磁控濺鍍。 排氣裴置:回轉泵+冷凍真空泵。 到達真空度:5. 3xl(T5[pa]。(Experiment to confirm the presence of hydrogen). The DC magnetron reduction of 4 inches: the sputtering target of the manufacturing example 13 is separately installed on the mining device, and the substrate temperature is room temperature (about 2 〇. 〇, the partial pressure of water is 〖. 〇 &gt;&lt; M /a (as an example), 5· 〇xl〇-3pa (as an example illusion and &amp; 〇χ 10 Pa (as a comparative example), three examples were prepared, examples, examples were prepared 2 and the transparent conductive film of Comparative Example 1. The conditions of the sputtering were as follows, and a film having a thickness of 1200 A was produced. The size of the bar was 0 = 4 in, t = 6 mm. The method of antimony mining: DC magnetron sputtering. Air entanglement: rotary pump + refrigerated vacuum pump. Reach vacuum: 5. 3xl (T5 [pa].

Ar 壓力:lOxlOlPa]。 氧氣壓力:〇 [pa]。 水壓力:1. Oxio-2、5. Oxio-3、5. 〇xl〇-5 [Pa]。 28 320646 200923973 , 基板溫度:室溫。 濺鍍電力:130W(電力密度1. 6W/ cm2)。 使用基板:C0RNING#1737(液晶顯示器用玻璃)、t=0· 8ram 此處’用膜xRD分析於各條件中經成膜之試料的結晶 狀,’破認在實施例1及實施例2中形成非晶型膜,於比 較例1中形成結晶化。 再者,關於各膜内氫之存在,使用飛行時間二次離子 f 質量分析法(T0F-SIMS、ULVAC PHI 公司製 TRIFT IV),關 於實施例1及比較例1之試料,藉由以下所表示之測定條 件’比較被檢驗出的(H+離子數)/(全部離子數)而確認。 [測定條件] 一次離子:Au +Ar pressure: lOxlOlPa]. Oxygen pressure: 〇 [pa]. Water pressure: 1. Oxio-2, 5. Oxio-3, 5. 〇xl〇-5 [Pa]. 28 320646 200923973 , substrate temperature: room temperature. Sputtering power: 130W (power density 1. 6W / cm2). Use substrate: C0RNING #1737 (glass for liquid crystal display), t=0·8 ram Here, 'the crystal shape of the sample formed by film formation in each condition was analyzed by film xRD, and it was broken in Example 1 and Example 2. An amorphous film was formed, and crystallization was formed in Comparative Example 1. Further, regarding the presence of hydrogen in each film, the time-of-flight secondary ion f mass spectrometry (T0F-SIMS, TRIFT IV manufactured by ULVAC PHI Co., Ltd.) was used, and the samples of Example 1 and Comparative Example 1 were represented by the following The measurement condition 'confirmed (H+ ion number) / (all ion number) was confirmed. [Measurement conditions] Primary ion: Au +

加速電壓:30KV 掃描條件:逐線掃描(raster-scan)(2〇〇χ2〇〇 # m) 於表8中’乃表示經成膜之試料T0F_SIMS分析結杲之 i (H+離子數)/(全部離子數)。 此處’成膜時之水之分壓為5· 0x1 (T5Pa與實際上在水 不存在的環境下成膜之參考試驗例3之試料中,被檢驗出 Η離子’可判斷為背景。亦即,於最近之研究中,被報導 由比參考試驗例3之水分壓更低的分壓成膜之氧化銦膜檢 驗出 Η +離子(JPn. J.Appl.Phys.Vol.46,No. 28,2007 ρρ. L685-L687),可推測被檢驗出之氫離子,於成膜時在基板 附著少許水分被取入膜内者。因此,本發明中,實質上水 不存在的環境下之水分壓為5. 0x10—5Pa以下之環境中成膜 29 320646 200923973 、 後之試樣之(H+離子數)/(全部離子數)之7. 75χ1(Γ4當作基 準值,較此增加之(Η +離子數)/(全部離子數)當作膜中含有 的氫離子。 於是,比較實施例及2與比較例1之(Η +離子之計 數V(全部離子之計數),得知成膜時之水分壓變大時亦隨之 變大。因此,誠如實施例1及2之方式,以控制成膜時之水 分壓,藉由於膜内取入氫,可確認變化之氫量。又,被取入 # 膜内的氫,因與膜内之原子的懸空鍵(dangl ing bond ;未結 合鍵)成為氫終端,推測其有妨礙膜的結晶化之效果。 [表8] 成膜時水分壓[pa] r離子數/全部離子數 測定結果 (測定結果)一(基準值) 實施例1 l.OxlO'2 9.18x1 (Γ4 1.43xl0_4 實施例2 5. OxlO'3 8. 98x10'4 1.23x10—4 比較例1 5. Oxl Ο'5 7. 75x10-4 0.00x10'° 【圖式簡單說明】 第1圖顯示本發明之試驗實施例A1至A18及A68至 A 7 3之結晶化溫度圖。 第2圖顯示本發明之試驗實施例B1至B18及B68至 B 7 3之結晶化溫度圖。 第3圖顯示本發明之參考試驗例C1至C73之結果圖。 【主要元件符號說明】 無 30 320646Acceleration voltage: 30KV Scanning conditions: raster-scan (2〇〇χ2〇〇# m) In Table 8, 'is the analyzed sample T0F_SIMS analysis of the knot i (H+ ion number) / ( All ion numbers). Here, the partial pressure of water at the time of film formation is 5.0·0x1 (in the sample of Reference Test Example 3 in which T5Pa is actually formed in an environment where water does not exist, the detected yttrium ion can be judged as the background. That is, in the recent study, it was reported that the indium oxide film was formed by a partial pressure film formed by a partial pressure lower than the water pressure of Reference Example 3 (JPn. J. Appl. Phys. Vol. 46, No. 28). , 2007 ρρ. L685-L687), it is presumed that the hydrogen ions to be detected are attached to the substrate with a small amount of water attached to the substrate during film formation. Therefore, in the present invention, the water is substantially in the absence of water. The pressure is 5. 0x10 - 5Pa or less in the environment of film formation 29 320646 200923973, the subsequent sample (H + ion number) / (all ions number) of 7. 75 χ 1 (Γ 4 as the reference value, compared to this increase (Η The number of ions + (the total number of ions) was taken as the hydrogen ion contained in the film. Thus, in Comparative Example 2 and Comparative Example 1, the count of V + ions (count of all ions) was observed. When the water pressure becomes large, it also becomes larger. Therefore, as in the methods of Examples 1 and 2, the water pressure at the time of film formation is controlled. The amount of hydrogen changed can be confirmed by taking hydrogen into the film. Further, the hydrogen taken into the film is hydrogen terminated by a dangling bond (unbonded bond) with an atom in the film. There is an effect of hindering the crystallization of the film. [Table 8] Water pressure at the time of film formation [pa] Number of r ions / total ion number measurement result (measurement result) 1 (reference value) Example 1 l. OxlO'2 9.18x1 ( Γ4 1.43xl0_4 Example 2 5. OxlO'3 8. 98x10'4 1.23x10-4 Comparative Example 1 5. Oxl Ο '5 7. 75x10-4 0.00x10'° [Simplified Schematic] FIG. 1 shows the present invention The crystallization temperature diagrams of Test Examples A1 to A18 and A68 to A 7 3 . Fig. 2 shows the crystallization temperature diagrams of Test Examples B1 to B18 and B68 to B 7 3 of the present invention. Fig. 3 shows the present invention. Refer to the results of test examples C1 to C73. [Main component symbol description] No 30 320646

Claims (1)

200923973 ·. 七、申凊專利範圍: 1· 一種透明導電膜’係使用具備氧化物婢处雕 臈為非晶形膜去,兮气札咕 凡、口贴之减錢乾成 :曰曰形膜者,该乳化物燒結體含有氧化 蚪3有鋇,該透明導電膜之特 、’同 , 時合右钼工, 寸厂文為3有乳化銦與錫且同 有鋇’而且㈣於銦1料之錫的料“:相料 於銦1莫耳之鋇的莫耳比以 為 ' ιλ-2Τ . Ν χ表不為未達(-2 9χ 〇 Ln(x)-6· 7χ1〇-2)之值,藉由曰 . 100°C以上。 人之、、口日日化溫度是 2.如申請專利範圍第^之透明 含有W圍弟1項之透明導電膜,其中該非晶型膜 I 專利範圍第2項之透明導電膜,其中該非晶型膜 5. 如申請專利範圍第丨至4 # ^ 項之透明導電膜,其 知於成胰後,藉由退火而結晶化之膜。 6. 如申睛專利範圍第5 ⑽至_t;進行。W其中該退火係於 7· 利範圍第5項之透明導電膜,其中該退火後之 月導-电膜之電阻率在5.0x10、.饳以下。 •利範圍第6項之透明導電膜,其中該退火後之 月K膜之電阻率在5.Gxl(r》咖以下。 月!電膜之製造方法’係使用具備氧化物燒結體 成版為非晶形膜’該氧化物燒結體含有氧化銦 320646 31 200923973 與錫且同時含有鋇’該透明導㈣之特徵為含 與錫且同時含有鋇,而且相對於銦1莫耳之錫的莫耳比 7:相2對於銦1莫耳之鋇的莫耳比以X表4未達(_2 9 xlO Ln(x)-6. 7x10 2)之值的非晶型膜於成膜時’成膜日卞 的水的分壓為l.0xl{r4Pa以上、1〇xi(rlpa以下。、可 10.如申請專利範圍第9項之透明導電膜的製造方法, 該非晶型膜藉由退火之結晶化溫度為⑽t以上。” 1.如申▲請專利範圍第9項之透明導電義製造方法, 其 成膜為非晶型膜後,藉由退火而為結晶化之膜。” •如申請專利範圍第10項之透明導電膜的製造方法 中^為非晶型膜後’藉由退火而為結晶化之膜。 其 :專利1已圍第11項之透明導電膜的製造方法 相由退火而為結晶化係於丨⑽至細。c進行。 其 •t申請專利範圍第12項之透明導電膜的製造方法 2猎由敎而為結晶化係於刚至縦C進行。 其 .中t利範㈣13項之透日轉電膜的製造方法,j 16 m明導電膜之電阻率在5n㈣下。 .=利_第14項之透料電膜的製造方法,复 中退火後之透明導電膜之電阻率在5. ㈣下、。 320646200923973 ·. VII. The scope of the patent application: 1. A transparent conductive film is made by using an oxide film to form an amorphous film, and the sputum is used to make money. The emulsion sintered body contains cerium oxide 3 and cerium, and the transparent conductive film has the characteristics of 'the same, the right and the right molybdenum, the inch is 3, the emulsified indium and tin have the same enthalpy' and (4) in the indium 1 The tin material of the material ": the molar ratio of the ingot to the indium 1 molar is 'ιλ-2Τ. Ν χ is not a failure (-2 9χ 〇Ln(x)-6· 7χ1〇-2) The value is 曰. 100 ° C or more. The daily temperature of the human, mouth is 2. The transparent conductive film containing one of the W brothers is transparent as in the patent application scope, wherein the amorphous film I patent The transparent conductive film of the second aspect, wherein the amorphous film 5. The transparent conductive film of the above-mentioned Patent Application No. 4 to 4, which is known as a film which is crystallized by annealing after being formed into a pancreas. For example, the scope of the patent application is carried out in the range of 5 (10) to _t; wherein the annealing is in the transparent conductive film of item 5 of the 7th item, wherein the month after the annealing is - The resistivity of the film is below 5.0x10, 饳. • The transparent conductive film of item 6 of the profit range, wherein the resistivity of the K film after the annealing is below 5. Gxl (r) coffee. The method 'is to use an oxide sintered body to form an amorphous film'. The oxide sintered body contains indium oxide 320646 31 200923973 and tin and contains 钡'. The transparent conductive layer (4) is characterized by containing tin and containing yttrium, and Mohr ratio 7 relative to indium 1 molar tin: phase 2 is inferior to the molar ratio of indium 1 molar to 0 (4 9 x lO Ln (x) - 6. 7 x 10 2) When the amorphous film is formed at the time of film formation, the partial pressure of the water of the film formation day is 1.0xl{r4Pa or more, 1〇xi (rpa below), and 10. The manufacture of the transparent conductive film of the ninth application patent scope The crystallization temperature of the amorphous film by annealing is (10) t or more. 1. The transparent conductive manufacturing method of the ninth patent of the patent application, which is formed into an amorphous film by annealing. It is a film which is crystallized." • In the manufacturing method of the transparent conductive film of claim 10, after the amorphous film is formed, The film is a crystallized film. The method for producing a transparent conductive film according to the eleventh item of Patent 1 is performed by annealing and crystallization is carried out from 丨(10) to fine c. The method for producing a transparent conductive film 2 is carried out by crystallization from the ruthenium to the 縦C. The method for producing a transflective film of the 13th item of the t-fan (4), the resistivity of the j 16 m conductive film is 5n (four) The manufacturing method of the transmissive electric film of the fourth item is the resistivity of the transparent conductive film after the intermediate annealing is 5. (4). 320646
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