TW200535275A - Method and apparatus for forming transparent conductive film - Google Patents

Method and apparatus for forming transparent conductive film Download PDF

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Publication number
TW200535275A
TW200535275A TW094104914A TW94104914A TW200535275A TW 200535275 A TW200535275 A TW 200535275A TW 094104914 A TW094104914 A TW 094104914A TW 94104914 A TW94104914 A TW 94104914A TW 200535275 A TW200535275 A TW 200535275A
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Taiwan
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film
gas
vapor
aforementioned
transparent conductive
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TW094104914A
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Chinese (zh)
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Toshiaki Sasaki
Kenji Yamamoto
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Kaneka Corp
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Publication of TW200535275A publication Critical patent/TW200535275A/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
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/455Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating characterised by the method used for introducing gases into reaction chamber or for modifying gas flows in reaction chamber
    • C23C16/45512Premixing before introduction in the reaction chamber
    • 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
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/22Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the deposition of inorganic material, other than metallic material
    • C23C16/30Deposition of compounds, mixtures or solid solutions, e.g. borides, carbides, nitrides
    • C23C16/40Oxides
    • C23C16/407Oxides of zinc, germanium, cadmium, indium, tin, thallium or bismuth
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/18Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
    • H01L31/1884Manufacture of transparent electrodes, e.g. TCO, ITO

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Organic Chemistry (AREA)
  • General Chemical & Material Sciences (AREA)
  • Metallurgy (AREA)
  • Mechanical Engineering (AREA)
  • Materials Engineering (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Physics & Mathematics (AREA)
  • Power Engineering (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Computer Hardware Design (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Manufacturing & Machinery (AREA)
  • Inorganic Chemistry (AREA)
  • Chemical Vapour Deposition (AREA)
  • Photovoltaic Devices (AREA)
  • Manufacturing Of Electric Cables (AREA)
  • Electrodes Of Semiconductors (AREA)

Abstract

Film forming equipment includes a film forming chamber (3) for depositing a transparent conductive film by CVD on a base (1) having an area of 220cm<SP>2</SP> or more, a first gas tube for transporting a first gas including organic metal vapor, a second gas tube for transporting a second gas including oxidant vapor, a gas mixing space (12) for mixing the first gas with the second gas by connecting the first and the second gas tubes, a gas introducing means (10) for introducing a reactive gas mixed in the gas mixing space into the film forming chamber, and an exhaust apparatus (6) for exhausting an exhaust gas from the film forming chamber.

Description

200535275 九、發明說明: 【發明所屬之技術領域】 本毛月係關於形成較大面積之透明導電膜用之方法及裝 遍種透明導電膜例如可適合利用於薄膜光電變換裝置 及:晶顯示裝置等。又,在本案專利說明書甲,有關半導 體薄膜之「晶質」與「微晶」之用詞如通常使用於該技術 頁或般亦可使用於局部地含有非晶質狀態之情形。 【先前技術】 一近年來,利用含有如多晶矽及微晶矽等晶質矽之薄膜之 ?電變換裝置之開發如火如荼地進行著。在此等光電變換 #置之開發t ’其目的在於藉較低溫處理在廉價基板上形 成良質之曰曰質矽之薄膜’以兼顧低廉化與高性能化。該種 光電變換裝置被期待應用於太陽電池及光感測器等各種用 途。 一般’為製作光電變換裝置’其—部分使用透明導電膜 為不可或缺。作為光電變換裝置之—例,已知有基本上具 有逐次形成含有由透明導電臈構成之表面電極、一導電型 層、晶質石夕系光電變換層及逆導電層之光電變換單元、含 :反射性金屬層之背面電極之構造之光電變換裳置。通 常,為更有效地利用入射於光電變換裝置之光,所採取之 在光入射側之表面電極設表面凹凸(表面紋理)構 4光散射至光電變換單元内,並使在背面金屬電極反射 之先進-步亂反射。又,為將光截留於光電變換單元内, Μ供有效利用,已知有將透明導電膜插入半導體層與背面 99619.d〇&lt; 200535275 電極間之裝置。另外,已知作為具有含pn或pin接合之多 數區域之疊層構造之串聯型光電變換裝置之中間層,含有 透明導電膜之裝置。 以往,在矽系薄膜光電變換裝置中,作為玻璃基板上之 透明導電膜,廣泛使用具有表面凹凸構造之氧化錫膜(例 如旭硝子公司製之U-type Sn〇2膜等)。但,該種氧化錫膜 在形成日守需要5 0 0 C以上之局溫處理,故成本較高。 作為使用規模較小之成膜裝置形成透明導電膜,尤其是 形成氧化鋅膜之方法,可利用高壓熱CVD(化學氣相沉 積)、真空蒸鍍、濺射、低壓熱CVD等方法。但,在高壓 熱CVD中,成膜溫度較高,故不能使用耐熱性低之玻璃或 塑膠膜等廉價基體,且在半導體膜構成之底層上形成透明 導電膜時,在該半導體膜中會發生缺陷及雜質擴散,對含 該半導體膜之特性之裝置特性帶來不良影響。在真空蒸鍍 ’但大面積之成膜較困200535275 IX. Description of the invention: [Technical field to which the invention belongs] The present invention relates to a method for forming a large-area transparent conductive film and the installation of the transparent conductive film. For example, it can be suitably used in thin-film photoelectric conversion devices and crystal display devices. Wait. In addition, in the patent specification A of this case, the terms "crystalline" and "microcrystalline" of a semiconductor thin film may be used in a case where the amorphous state is partially contained if it is generally used on the technical page. [Previous Technology] In recent years, the development of electrical conversion devices using thin films containing crystalline silicon such as polycrystalline silicon and microcrystalline silicon has been in full swing. The purpose of these photoelectric conversions is to develop low-temperature processing to form a good-quality silicon thin film on a low-cost substrate to achieve both low cost and high performance. This type of photoelectric conversion device is expected to be used in various applications such as solar cells and light sensors. In general, it is indispensable to use a transparent conductive film for the manufacture of a photoelectric conversion device. As an example of a photoelectric conversion device, it is known to basically have a photoelectric conversion unit that successively forms a surface electrode composed of a transparent conductive plutonium, a conductive type layer, a crystalline stone-based photoelectric conversion layer, and a reverse conductive layer, including: Photoelectric conversion structure of the back electrode of the reflective metal layer. In general, in order to use the light incident on the photoelectric conversion device more effectively, the surface electrode on the light incident side is provided with a surface unevenness (surface texture) structure to diffuse the light into the photoelectric conversion unit and reflect the metal electrode on the back side. Advanced-step chaos reflection. Further, in order to trap light in the photoelectric conversion unit and effectively use M, a device is known in which a transparent conductive film is inserted between the semiconductor layer and the back surface 99619.d0 &lt; 200535275 electrode. In addition, a device including a transparent conductive film is known as an intermediate layer of a tandem-type photoelectric conversion device having a multilayer structure including a plurality of regions including pn or pin junctions. Conventionally, in a silicon-based thin-film photoelectric conversion device, as a transparent conductive film on a glass substrate, a tin oxide film (for example, a U-type Sn02 film manufactured by Asahi Glass Co., Ltd.) has been widely used as a transparent conductive film on a glass substrate. However, this kind of tin oxide film needs to be treated at a local temperature of more than 500 ° C during the formation of the sun guard, so the cost is higher. As a method for forming a transparent conductive film using a small-scale film-forming device, especially a zinc oxide film, methods such as high-pressure thermal CVD (chemical vapor deposition), vacuum evaporation, sputtering, and low-pressure thermal CVD can be used. However, in high-pressure thermal CVD, the film formation temperature is high, so inexpensive substrates such as glass or plastic films with low heat resistance cannot be used, and when a transparent conductive film is formed on the bottom layer of a semiconductor film, it will occur in the semiconductor film. Defects and impurity diffusion adversely affect device characteristics including the characteristics of the semiconductor film. Under vacuum evaporation ’but the film formation on a large area is difficult

中,雖可用較低溫沉積透明導電膜,令 難,且成膜速度較慢。利用濺射法時, 積透明導電膜,但由於搡用由釦矣而¥Medium, although it is possible to deposit a transparent conductive film at a lower temperature, it is difficult and the film formation speed is slow. When the sputtering method is used, a transparent conductive film is deposited.

法(或稱MOCVD(有機金屬CVD)法)。 劑蒸氣之低壓熱c VD 在圖20之概念圖中, 99619.doc 200535275 表示Wilson W· Wenas等在非專利文獻}所揭示之利用典型 的低壓熱CVD法之氧化鋅膜之沉積裝置作為先行例。在此 成膜裝置中,真空槽4之内部為設置基板1之成膜室3。作 為含鋅之有機金屬蒸氣,將二乙基鋅(DEZ)蒸氣在與Ar載 氣混合之狀態通過DEZ供應管7供應至成膜室3。同樣地將 氧化劑蒸氣之水(ho)蒸氣在與^載氣混合之狀態通過出〇 供應管8供應至成膜室3。 在此,將有機金屬蒸氣與氧化劑蒸氣分別經由個別之氣 體供應管7、8導入成膜室3之理由在於以同一氣體導入管 輸送有機金屬蒸氣與氧化劑蒸氣時,在至成膜室前會在該 氣體導入管内起反應,該氣體導入管會在短時間内被反應 沉積物所阻塞之故。 在成膜至3内,例如玻璃基板1被加熱器2加熱而被施行 低壓熱CVD,藉以在玻璃基板丨之表面上沉積氧化錫膜作 為透明導電膜,成膜時之基板溫度設定於100°C〜300。〇之 範圍内,壓力設定於!至25 t〇rr(133 pa〜3325以)之範圍 内,成膜至3内之反應後之廢氣由排氣口 5及排氣管6被排 出依據此成膜方法,透明導電膜之沉積時之底層溫度較 低,故可使用玻璃等廉價之底層。又,在原理上不會產生 女歲射法之情形般之離子,故在作為底層之基體或半導體 層,也不會發生離子造成之損傷。 為幵/成大面積之透明導電膜,而利用典型地如圖2〇 斤丁之先行例時,所沉積之大面積之透明導電膜之面内均 句性部成問題。即,為以低壓熱CVD沉積大面積且均勻之 99619.doc 200535275 透明導電膜,有必要對大面積之底層上均勻地供應有機金 屬蒸氣與氧化劑蒸氣,且由該處排氣。但在圖20中,由於 DEZ與H20係分別由氣體供應管7、8個別地被導入成膜室3 内,故難以在大面積之基體1之表面上均勻供應DEZ與 H20。其結果,難以保持所沉積之大面積之透明導電膜之 厚度及物性之均勻性。 [非專利文獻 1] Wilson W. Wenas,Akira Yamada,Makoto Konagai and Kiyoshi Takahashi; &quot;Textured ZnO Thin Film for Solar Cells Grown by Metalorganic Chemical Vapor Deposition’’,Jpn. J. Appl. Phys·,Vol· 30,No. 3B,March 1991,pp. L441-L443. 【發明内容】 有鑑於上述先行例之課題,本發明之目的係在使用有機 金屬蒸氣與氧化劑蒸氣之低壓熱CVD中,提供一種形成大 面積且均勻之透明導電膜之方法及裝置。且亦以提供含該 大面積之透明導電膜之裝置,例如大面積之光電變換裝置 或液晶顯示裝置等為目的。 本發明之成膜裝置係包含利用CVD將透明導電膜沉積於 具有220 cm2以上之面積之底層上用之成膜室、輸送含有 機金屬蒸氣之第1氣體之第1氣體管、輸送含氧化劑蒸氣之 第2氣體之第2氣體管、結合第1與第2氣體管以混合第1與 第2氣體用之氣體混合空間、將在該氣體混合空間被混合 之反應氣體導入成膜室内之氣體導入手段及由成膜室排出 排氣用之排氣裝置。 99619.doc 200535275 即,在導入於配置底層之成膜室前,藉混合有機金屬蒸 ^與氧化劑蒸氣,可在該底層上沉積大面積且均勻之透明 導電膜。又,藉將含有機金屬蒸氣與氧化劑蒸氣之反應氣 體以噴淋狀導入成膜室内,可更進一步提高大面積之透明 導電膜之均勻性。 但在導入於成膜室前,若在加熱至例如約㈣之外徑 1/4叶(内徑約4·4 mm)之配管内混合有機金屬蒸氣之二乙: 鋅蒸氣與氧化劑蒸氣之水蒸氣時, 土 — 丁幻在δ亥配官中有機金屬 洛氣與氧化劑蒸氣之反應開始後透明導電膜或粉體合沉積 於配管中’在短時間内該配管會閉塞。具體而言,在玻璃 基板上沉積厚度約丨障之氧化鋅膜所需之時間内配管會閉 塞’錢即不能成膜。又,需要將配管加熱係為防止:乙 基辞蒸氣或水蒸氣液化之故。 树明人詳細調查有機金屬蒸氣與氧化劑蒸氣之反應條 ,糟此务現-種可獲得在工業上可容許混合有機金屬基 乳人乳化劑蒸氣後至配管閉塞以前之時間之範圍之條件。 具體而言’將混合有機金屬蒸氣與氧化劑蒸氣之空間及由 該處向成膜室内導人反應氣体之路徑之壁面溫度控制 =範圍’藉此可抑制配管閉塞。又,充分增大混合有機 金屬蒸亂與乳化劑蒸氣之空間及由該處向成膜室内導 應氣体之路徑之剖面積,即增大配管之氣流傳導以降低其 内壓力,藉此可抑制該配管之閉塞。因此,依據本發明^ 决之速度》儿積大面積且均勾之透明導電膜而不合 a與作為底層之基體或半導體層不良影響。 曰 99619.doc 200535275 【發明之效果】 :以上所述,依據本發明,在制有機金屬蒸氣與氧化 叙氣之低壓熱CVD中,可形成大面積且均句之透明導電 膜。其結果,可製作含大面積之透明導電膜之大面積之裝 置,尤其是製作大面積之光電變換襄置,並提高其特性。、 【實施方式】 首先’使用液體材料作為成膜用氣體之原料時,最好以 起泡氣化器或喷霧氣化器將該液體材料之至少一種氣化。 使用DEZ蒸氣作為有機金屬蒸氣,使用H2〇蒸氣作為氧化 劑蒸氣時,將液體狀態之DEZ與仏〇氣化使用。為混合此 f蒸氣,有必要使DEZ之氣化器之出口壓力與H2〇之氣化 器之出口Μ力大致相等。兩者麼力有大差異時,壓力低之 蒸氣會被推回而使流量不穩定或無法流出。 蒸氣氣化器之出口壓力決定於液體材料之蒸氣壓,故難 以控制其出口壓力。使用蒸氣氣化器時,若在將Μζ蒸氣 與札〇蒸氣導入成膜室前混合時,因DEZ蒸氣低於札〇蒸 氣,有發生DEZ蒸氣會被推回而無法流出之問題。 使用起泡氣化器或喷霧氣化器時,在成膜室内之壓力一 定時,氣化器之出口壓力大致決定於載氣之壓力,故可調 整氣化器之出口壓力。另外,為抑制在氣體混合空間丨2之 粉體之產生(參照圖5),氣化器、DEZ供應管7、及H20供 應管8之溫度最好儘可能地低。基於此理由,以使用較低 溫之起泡氣化器或喷霧氣化器為宜。 圖23係蒸發氣化器之概念圖。以加熱器26加熱裝入液體 99619.doc -10- 200535275 材料28之槽27而產生蒸氣29,使該液體材料氣化。氣化之 氣體之質量被氣體質量流控制器30定量地控制及供應。此 氣體貝里 控制^§ 3 0也必要在入口與出口之差壓在〇 〇 5 MPa下仍能啟動’其價格高於以一般的Mpa#上之差 壓起動之負置流控制器。蒸氣氣化器之出口壓力決定於液 體材料之蒸氣壓,故控制較為困難。因此,在進入成膜室 前,混合有機金屬蒸氣與氧化劑蒸氣並不容易。 圖24係起泡氣化器之概念圖。將Ar載氣通至液體材料28 中以產生氣泡33,藉以使該液體材料氣化。Ar一面被氣體 質ΐ流控制器34控制流量,一面被供應。此氣體質量流控 制器34係以0.05 MPa以上之差壓起動之一般的質量流控制 器。將槽27裝入恆溫槽32而將其溫度控制於一定。Ar與氣 化之氣體混合後由起泡氣化器之出口流出。被起泡氣化器 氣化之氣體流量決定於Ar流量、液體材料之溫度、液面高 度等,難以定量地加以控制。從重量計31所測定之槽27與 液體材料28之合計重量之減少中,可測定氣化之液體材料 之虿之大略值。起泡氣化器之出口壓力大致決定於載氣之 壓力,可加以控制。因此,在進入成膜室前,可混合有機 金屬蒸氣與氧化劑蒸氣。 在圖25中’(a)係噴霧氣化器之全體的概念圖,(b)係更 洋、、、田ί、、員示(a)所含之混合器36之放大概念圖。一面以氣體質 篁流控制34控制Ar載氣流量而加以供應,一面以液體質 量流控制器35控制液體材料流量而加以供應,在混合器% 此合此等而使其氣化。如圖25⑻所示,由副共應管3了供 99619.doc -11 - 200535275 應Ar氣。液體材料係通過液體材料供應管38而由微小孔39 被供應作為霧狀液體材料40。霧狀液體材料40被強勢流出 之Ar氣所氣化後,被氣化氣體供應管41導出。喷霧氣化器 之出口壓力大致決定於載氣之壓力,故可加以控制。因 • 此’可在進入成膜室前,混合有機金屬蒸氣與氧化劑蒸 氣。又,因通過液體質量流控制器35之液體材料全部被氣 化,故可施行氣化之氣體之定量控制。又,噴霧氣化器雖 比起泡氣化器昂責,但比蒸發氣化器低廉。 • 圖5之概念圖係表示本發明之一實施例之透明導電膜之 形成方法。在本圖中,真空槽4之内部係配置基板1之成膜 室3。將含辞之有機金屬蒸氣之二乙基鋅(DEZ)蒸氣在與Ar 載氣混合之狀態下供應至氣體混合空間12,將氧化劑蒸氣 之水(KUO)蒸氣在與Ar載氣混合之狀態下供應至氣體混合 空間12,藉以在氣體混合空間12内調製含deZ、h2〇、Ar 之反應氣體。 在圖21之模式圖中’氣體混合空間附近之配管之一例。 癱 在此圖中,在DEZ供應管7與Η2〇供應管8之合流位置以虛 線圍成之區域為氣體混合空間12。DEZ供應管7被加熱器 71加熱,HW供應管被加熱器§ 1加熱。在氣體混合空間J 2 内調製之反應氣體係被反應器體配管丨丨導向成膜室3。 DEZ瘵氣與蒸氣之合流位置雖為氣體混合空間丨2, 但實際上因擴散而在DEZ供應管7存在著某種程度之h2〇蒸 氣’反之’在H2〇供應管8中存在著某種程度之DEZ蒸氣。 因此,DEZ供應管7與He供應管8中可產生Zn〇之粉體。 99619.doc 12 200535275 與配管相比,若將氣流導動性小之閥配置於氣體混合空間 12附近’則該閥在短時間會被產生之粉體閉塞。 因此’由氣體混合空間12向上流側設於DEZ供應管7之 ’ 最初之DEZ供應閥24以與氣體混合空間12距離〇·3 m以上 &quot; (圖2 1中之距離A)較為理想,距離1 ηι以上更為理想。同樣 地’由氣體混合空間12向上流側設於h2〇供應管8之最初之 供應閥25以與氣體混合空間12距離0.3 m以上(圖21中 之距離B)較為理想,距離1 m以上更為理想。 • DEZ供應管7中之私0密度可利用下式1之擴散方程式計 算: D · a2 NH/a x2-k · nh · Nd=0 (式 1) 在此,D為H20之擴散常數,NH為H20之分子數密度,x為 由氣體混合空間12沿著DEZ供應管7之距離,k為DEZ蒸氣 與H20蒸氣之反應速度常數,ND為DEZ蒸氣之分子數密 度。解式1,可得下式2: NH= NH0 · exp[-/~{ k · ND/ (NH0 · D)} · X](式 2) W 在此,NH0為在氣體混合空間12之H20分子數密度。 圖22之曲線係表示式2之計算結果之一例。此曲線之橫 軸係表示由混合空間12沿著DEZ供應管7之距離X,縱軸係 表示氣體混合空間12中之H20濃度為1時之距離X之H20相 對密度。此時,氣體混合空間12中之DEZ蒸氣之分壓為75 Pa,H20蒸氣之分壓為75 Pa。又,假定由分子量概算之 H20之擴散速度D=0.01 m2/s,假定由ZnO之成膜速度概算 之反應速度常數k=1.3xl(T28m3/s。 99619.doc -13- 200535275 由圖22可知··對氣體混合空間12中之h2〇濃度,距離乂在 0.3 m以上時’ Ηβ相對濃度在1%以下,在χ=;ι _寺,不足 1 ppm。即,如上所述,由氣體混合空間12至DEZ供應閥 24之距離A在0.3 m以上時,可抑制Zn〇粉體之產生而防止 閥之阻基,在1 m以上時更為理想。在H2〇供應管82DEZ 派度也對距離成對數性的減少,故由氣體混合空間12至 H2〇供應閥25之距離A在0.3 m以上時較為理想,在i m以上 時更為理想。Method (also known as MOCVD (Organic Metal CVD) method). Low-pressure thermal c VD of agent vapor In the conceptual diagram of Fig. 20, 99619.doc 200535275 represents a deposition device using a typical low-pressure thermal CVD method of zinc oxide film disclosed by Wilson W. Wenas et al. In a non-patent document}. . In this film forming apparatus, the inside of the vacuum chamber 4 is a film forming chamber 3 in which the substrate 1 is installed. As the zinc-containing organometal vapor, diethylzinc (DEZ) vapor is supplied to the film forming chamber 3 through a DEZ supply pipe 7 in a state of being mixed with an Ar carrier gas. Similarly, the water (ho) vapor of the oxidant vapor is supplied to the film forming chamber 3 through the outlet tube 8 in a state of being mixed with the carrier gas. Here, the reason why the organometal vapor and the oxidant vapor are introduced into the film formation chamber 3 through separate gas supply pipes 7 and 8 is that when the organometal vapor and the oxidant vapor are transported through the same gas introduction pipe, the The gas introduction tube reacts, and the gas introduction tube will be blocked by the reaction deposit in a short time. Within film formation 3, for example, the glass substrate 1 is heated by the heater 2 and subjected to low-pressure thermal CVD, so that a tin oxide film is deposited on the surface of the glass substrate as a transparent conductive film, and the substrate temperature during film formation is set at 100 ° C ~ 300. Within the range of 〇, the pressure is set at! In the range of 25 t〇rr (133 pa to 3325), the exhaust gas after the reaction from film formation to 3 is discharged from the exhaust port 5 and the exhaust pipe 6 According to this film formation method, when the transparent conductive film is deposited The temperature of the bottom layer is relatively low, so a cheap bottom layer such as glass can be used. In addition, in principle, no ion like that in the case of female shooting is generated, so no damage caused by ions will occur in the substrate or semiconductor layer as the bottom layer. In order to form a large-area transparent conductive film, when using the precedent typically as shown in FIG. 20, the deposited large-area transparent conductive film has a problem in the plane of the sentence. That is, in order to deposit a large-area and uniform 99619.doc 200535275 transparent conductive film by low-pressure thermal CVD, it is necessary to uniformly supply organic metal vapor and oxidant vapor to a large-area bottom layer, and exhaust the gas from there. However, in FIG. 20, since DEZ and H20 are respectively introduced into the film forming chamber 3 by the gas supply pipes 7, 8 respectively, it is difficult to uniformly supply DEZ and H20 on the surface of the substrate 1 with a large area. As a result, it is difficult to maintain the uniformity of the thickness and physical properties of the deposited large-area transparent conductive film. [Non-Patent Document 1] Wilson W. Wenas, Akira Yamada, Makoto Konagai and Kiyoshi Takahashi; &quot; Textured ZnO Thin Film for Solar Cells Grown by Metalorganic Chemical Vapor Deposition '', Jpn. J. Appl. Phys ·, Vol · 30 , No. 3B, March 1991, pp. L441-L443. [Summary of the Invention] In view of the problems of the foregoing precedents, the object of the present invention is to provide a method for forming a large area in low-pressure thermal CVD using an organometal vapor and an oxidant vapor. Method and device for uniform and transparent conductive film. It is also intended to provide a device including the large-area transparent conductive film, such as a large-area photoelectric conversion device or a liquid crystal display device. The film-forming device of the present invention includes a film-forming chamber for depositing a transparent conductive film on a bottom layer having an area of 220 cm2 or more by CVD, a first gas pipe for conveying a first gas containing organic metal vapor, and a vapor containing oxidant A second gas pipe of the second gas, a gas mixing space for combining the first and second gas pipes to mix the first and second gases, and a gas introduction for introducing a reaction gas mixed in the gas mixing space into the film forming chamber Means and exhaust device for exhausting exhaust from film-forming chamber. 99619.doc 200535275 That is, before introducing into the film forming chamber with the bottom layer, by mixing organic metal vapor and oxidant vapor, a large area and uniform transparent conductive film can be deposited on the bottom layer. In addition, by introducing the reaction gas containing organic metal vapor and oxidant vapor into the film forming chamber in a spray shape, the uniformity of a large-area transparent conductive film can be further improved. However, before being introduced into the film forming chamber, if the organic metal vapor is mixed in a pipe heated to, for example, an outer diameter of 1/4 leaf (inner diameter of approximately 4 · 4 mm): water of zinc vapor and oxidant vapor In the case of steam, when the reaction of the organometallic gas and the oxidant vapor in the δ-Hai formulation begins, a transparent conductive film or powder is deposited in the piping, and the piping will be blocked in a short time. Specifically, the piping will be blocked within a period of time required to deposit a zinc oxide film having a thickness of about 200 Å on the glass substrate, and the film cannot be formed. In addition, the piping needs to be heated to prevent liquefaction of ethyl vapor or water vapor. Shu Mingren investigated in detail the reaction strips of organometallic vapors and oxidant vapors. This problem is now a condition that can be obtained in the industrially acceptable time range after the mixing of organometallic emulsifier vapors before the piping is blocked. Specifically, 'the wall temperature control of the space in which the organometal vapor and the oxidant vapor are mixed and the path from which the reaction gas is introduced into the film forming chamber = range' can be used to suppress occlusion of the pipe. In addition, the space for mixing the organometallic steaming and emulsifier vapor and the cross-sectional area of the path for conducting gas to the film-forming chamber from this place are sufficiently increased, that is, the airflow conduction of the pipe is increased to reduce the internal pressure, thereby suppressing the internal pressure. The piping is blocked. Therefore, according to the present invention, the "determined speed" of the transparent conductive film with a large area and uniformity does not affect a substrate or a semiconductor layer as a bottom layer. 99619.doc 200535275 [Effect of the invention]: As mentioned above, according to the present invention, a large-area and uniform uniform transparent conductive film can be formed in low-pressure thermal CVD for the production of organometal vapor and oxidation gas. As a result, a large-area device including a large-area transparent conductive film can be produced, particularly a large-area photoelectric conversion device, and its characteristics can be improved. [Embodiment] First, when a liquid material is used as a raw material for a film-forming gas, it is preferable to vaporize at least one of the liquid materials with a bubble gasifier or a spray gasifier. When DEZ vapor is used as the organometal vapor and H2O vapor is used as the oxidant vapor, DEZ and ZO in the liquid state are vaporized and used. In order to mix this f vapor, it is necessary to make the outlet pressure of the DEZ gasifier approximately equal to the outlet M force of the H2O gasifier. When there is a big difference between the two forces, the low-pressure steam will be pushed back, making the flow unstable or unable to flow out. The outlet pressure of a vapor gasifier is determined by the vapor pressure of the liquid material, so it is difficult to control its outlet pressure. When a vaporizer is used, if the MZ vapor is mixed with the Zao vapor before being introduced into the film forming chamber, the DEZ vapor is lower than the Zao vapor, and there is a problem that the DEZ vapor is pushed back and cannot flow out. When using a bubble gasifier or a spray gasifier, the outlet pressure of the gasifier is approximately determined by the pressure of the carrier gas at a certain time in the pressure of the film forming chamber, so the outlet pressure of the gasifier can be adjusted. In addition, in order to suppress the generation of powder in the gas mixing space 2 (see FIG. 5), the temperature of the gasifier, the DEZ supply pipe 7, and the H20 supply pipe 8 should preferably be as low as possible. For this reason, it is advisable to use a lower temperature foaming gasifier or spray gasifier. Figure 23 is a conceptual diagram of an evaporative gasifier. The heater 26 is used to fill the liquid 99619.doc -10- 200535275 and the groove 27 of the material 28 generates vapor 29 to vaporize the liquid material. The mass of the gasified gas is quantitatively controlled and supplied by the gas mass flow controller 30. This gas Bailey control ^ § 30 also needs to be able to start at the differential pressure between the inlet and outlet at 0.05 MPa. Its price is higher than a negative flow controller that starts with a differential pressure on the general Mpa #. The outlet pressure of the vapor gasifier is determined by the vapor pressure of the liquid material, so it is difficult to control. Therefore, it is not easy to mix the organometallic vapor and the oxidant vapor before entering the film forming chamber. Figure 24 is a conceptual diagram of a bubble gasifier. The Ar carrier gas is passed into the liquid material 28 to generate bubbles 33, thereby vaporizing the liquid material. Ar is supplied while the flow is controlled by the gas mass flow controller 34. This gas mass flow controller 34 is a general mass flow controller which is started at a differential pressure of 0.05 MPa or more. The tank 27 is set in the thermostatic tank 32 and the temperature thereof is controlled to be constant. Ar is mixed with the gasified gas and flows out from the outlet of the bubble gasifier. The gas flow rate gasified by the bubbling gasifier is determined by the Ar flow rate, the temperature of the liquid material, the liquid level height, etc., and it is difficult to control quantitatively. From the reduction in the total weight of the groove 27 and the liquid material 28 measured by the weight gauge 31, the approximate value of the vaporized liquid material can be determined. The outlet pressure of the bubble gasifier is roughly determined by the pressure of the carrier gas and can be controlled. Therefore, before entering the film forming chamber, an organometal vapor and an oxidant vapor may be mixed. In Fig. 25, '(a) is a conceptual diagram of the entire spray gasifier, and (b) is an enlarged conceptual diagram of the mixer 36 included in the more advanced, high-tech, high-tech, high-tech, low-tech (36). While supplying the Ar carrier gas flow rate by the gas mass flow control 34, the liquid material flow rate is controlled by the liquid mass flow controller 35 while supplying it, and the mixer is combined to vaporize it. As shown in Fig. 25 (a), the vice coordinator 3 supplies 99619.doc -11-200535275 for Ar gas. The liquid material is supplied as a mist-like liquid material 40 through a micro hole 39 through a liquid material supply pipe 38. The atomized liquid material 40 is gasified by the strongly flowing Ar gas, and is then led out by the gasified gas supply pipe 41. The outlet pressure of the spray gasifier is roughly determined by the pressure of the carrier gas, so it can be controlled. Therefore, 'the organic metal vapor and the oxidant vapor can be mixed before entering the film forming chamber. In addition, since all the liquid materials passing through the liquid mass flow controller 35 are vaporized, quantitative control of the vaporized gas can be performed. In addition, the spray gasifier is more expensive than the bubble gasifier, but it is cheaper than the evaporative gasifier. • The conceptual diagram of FIG. 5 shows a method for forming a transparent conductive film according to an embodiment of the present invention. In this figure, a film-forming chamber 3 of a substrate 1 is arranged inside the vacuum chamber 4. Diethyl zinc (DEZ) vapor containing organic metal vapor is supplied to the gas mixing space 12 in a state mixed with an Ar carrier gas, and water (KUO) vapor of an oxidant vapor is mixed with an Ar carrier gas It is supplied to the gas mixing space 12, thereby preparing a reaction gas containing deZ, h2O, and Ar in the gas mixing space 12. An example of the piping near the 'gas mixing space' in the schematic diagram of FIG. 21. Paralysis In this figure, the area surrounded by the dotted line at the confluence position of the DEZ supply pipe 7 and the Η20 supply pipe 8 is the gas mixing space 12. The DEZ supply pipe 7 is heated by the heater 71, and the HW supply pipe is heated by the heater §1. The reaction gas system prepared in the gas mixing space J 2 is guided by the reactor body pipe 丨 丨 to the film forming chamber 3. Although the confluence position of DEZ radon and steam is a gas mixing space 2, in fact, there is a certain degree of h2O vapor in the DEZ supply pipe 7 due to diffusion. There is some kind of H2O supply in 8 Degree of DEZ vapor. Therefore, ZnO powder can be generated in the DEZ supply pipe 7 and the He supply pipe 8. 99619.doc 12 200535275 Compared with piping, if a valve with low airflow conductivity is arranged near the gas mixing space 12 ', the valve will be blocked by the generated powder in a short time. Therefore, “the gas mixing space 12 is provided on the upstream side of the DEZ supply pipe 7” The initial DEZ supply valve 24 is preferably at a distance of 0.3 m or more from the gas mixing space 12 (distance A in FIG. 21), A distance of 1 η or more is more ideal. Similarly, the initial supply valve 25 provided on the upstream side of the h2O supply pipe 8 from the gas mixing space 12 is preferably at a distance of 0.3 m or more from the gas mixing space 12 (distance B in FIG. 21), and more preferably at a distance of 1 m or more. As ideal. • The density of the private 0 in the DEZ supply pipe 7 can be calculated using the following diffusion equation: D · a2 NH / a x2-k · nh · Nd = 0 (Equation 1) Here, D is the diffusion constant of H20, NH Is the molecular number density of H20, x is the distance from the gas mixing space 12 along the DEZ supply pipe 7, k is the reaction rate constant of DEZ vapor and H20 vapor, and ND is the molecular number density of DEZ vapor. Solving formula 1 gives the following formula: NH = NH0 · exp [-/ ~ {k · ND / (NH0 · D)} · X] (Equation 2) W Here, NH0 is H20 in the gas mixing space 12 Molecular number density. The graph in FIG. 22 shows an example of the calculation result of Expression 2. The horizontal axis of this curve represents the distance X from the mixing space 12 along the DEZ supply pipe 7, and the vertical axis represents the relative density of H20 at the distance X when the H20 concentration in the gas mixing space 12 is 1. At this time, the partial pressure of the DEZ vapor in the gas mixing space 12 is 75 Pa, and the partial pressure of the H20 vapor is 75 Pa. It is assumed that the diffusion rate D of H20 estimated from the molecular weight is D = 0.01 m2 / s, and the reaction rate constant k estimated from the film-forming speed of ZnO is k = 1.3xl (T28m3 / s. 99619.doc -13- 200535275). · For the concentration of h20 in the gas mixing space 12, when the distance 乂 is greater than 0.3 m, the relative concentration of Ηβ is less than 1%, and is less than 1 ppm at χ =; ι _ temple. That is, as described above, mixed by the gas When the distance A from the space 12 to the DEZ supply valve 24 is more than 0.3 m, it can suppress the generation of Zn0 powder and prevent the resistance of the valve. It is more ideal when it is more than 1 m. In the H2O supply pipe 82DEZ, the degree is also correct. The distance decreases logarithmically, so the distance A from the gas mixing space 12 to the H2O supply valve 25 is more than 0.3 m, and more preferably, it is more than im.

在氣體混合空間12内調製之反應氣體經由反應氣配管 11、擴散相9、與噴淋板1〇構成之反應氣體經路而被供應 至成膜室3。反應氣體由設於噴淋板1〇之多數孔以喷淋狀 喷出,均勻地供應至成膜室3内。氣體混合空間丨2之壁面 及反應氣體經路(反應氣配管U、擴散箱9、及與喷淋板1〇) 之壁面被壁面加熱器&quot;控制溫度。玻璃基板i被加熱器2加 熱以施行低壓熱CVD,在基板面上沉積作為透明導電膜之 氧化鋅膜。作為加熱器2,例如可使用鎧裝加熱器。廢氣 經由排氣口 5及排氣管6而被泵(未圖示)排出。且可利用未 表示於圖5之電容壓力計與電容可變閥,將真空槽4中之壓 力保持於一定。沉積氧化辞膜時,例如可設定為:真空槽 4之壓力5〜200 Pa、基板溫度1〇〇〜3〇〇t、dez蒸氣流量 10〜1000 seem、H2〇蒸氣流量1〇〜1〇〇〇 sccm以及&amp;流量 100〜10000 seem之範圍内。 在圖5之實施型態中,不僅真空槽4外之氣體混合空間η 之壁面’連向真空槽4内突出之反應氣體經路9、ι〇之壁面 99619.doc -14· 200535275 也叉到溫度控制。另一方面, ^ ^ ^ Α 傻述之比較例1或3中,在 反應氣體經路中,僅將真空槽外 片、 卜之部分加熱至約80〇C 〇 氣體混合空間或反應氣體經路 路之壁面溫度過高時,在 處,有機金屬蒸氣與氧化劑蒸氧 “、、乳會起反應,沉積透明導雷 膜或粉體而發生閉塞。又,氣, ”工ώ &amp;體混合空間或反應氣體經路 之壁面溫度過低時,難以維持卓 f車乂呵之有機金屬蒸氣與氧化 W蒸氣之瘵氣壓,最惡劣時可能 丁』此發生液化。為避免此現 象,控制壁面加熱器13,將氣體混人处The reaction gas prepared in the gas mixing space 12 is supplied to the film formation chamber 3 via a reaction gas pipe 11, a diffusion phase 9, and a reaction gas formed by the shower plate 10. The reaction gas is sprayed from a plurality of holes provided in the shower plate 10 in a shower shape, and is uniformly supplied into the film forming chamber 3. The wall surface of the gas mixing space 2 and the wall surface of the reaction gas path (reaction gas piping U, the diffusion box 9, and the shower plate 10) are controlled by a wall surface heater &quot;. The glass substrate i is heated by the heater 2 to perform low-pressure thermal CVD, and a zinc oxide film as a transparent conductive film is deposited on the substrate surface. As the heater 2, for example, an armored heater can be used. The exhaust gas is discharged by a pump (not shown) through an exhaust port 5 and an exhaust pipe 6. The capacitance pressure gauge and the capacitance variable valve (not shown in Fig. 5) can be used to keep the pressure in the vacuum tank 4 constant. When depositing the oxide film, for example, the pressure in the vacuum tank 4 can be set to 5 to 200 Pa, the substrate temperature can be 100 to 300 t, the dez vapor flow rate can be 10 to 1000 seem, and the H2O vapor flow rate can be 10 to 100. 〇sccm and &amp; flow range 100 ~ 10000 seem. In the embodiment shown in FIG. 5, not only the wall surface of the gas mixing space η outside the vacuum tank 4 but also the wall surface of the reaction gas passage 9 and ι〇 protruding in the vacuum tank 4 are 99,619.doc-14.200535275. temperature control. On the other hand, ^ ^ ^ Α In Comparative Example 1 or 3 described succinctly, in the reaction gas path, only the outer part of the vacuum tank and the part are heated to about 80 ° C. The gas mixing space or the reaction gas path When the temperature of the wall surface of the road is too high, everywhere, organometallic vapors and oxidants vaporize oxygen, and milk reacts, and a transparent lightning film or powder is deposited to cause occlusion. Also, gas, “industrial &amp; body mixing space Or, if the temperature of the wall surface of the reaction gas path is too low, it is difficult to maintain the pressure of the organic metal vapor and the oxidized W vapor of the car, and liquefaction may occur in the worst case. To avoid this, control the wall heater 13 to mix the gas

此ϋ工間及反應氣體經路 之壁面之至少-方之至少-部份之溫度控制㈣〜⑽。c, 較好控制於50〜8(TC,最好控制於55〜6代之範圍。作為辟 面加熱器13,可利用例如電阻加熱式之加熱器(鐘裝加教 器:帶狀加熱器、矽橡膠加熱器)、紅外線加熱器、溫媒 循環加熱器(使加熱之油或水等流體循環之加熱器)等。 氣體混合空間或反應氣體經路之剖面積小時,氣流導動 性變小,與成膜室内之壓力相比,氣體混合空間或反應氣 體經路之壓力會變得非常高。此時,在氣體混合空間混合 DEZ與HA時,配管中會產生膜及粉體而在短時間發生閉 塞。 為避免配管之閉塞,在本發明中,將氣體混合空間與反 應氣體經路之氣流剖面積設定於28 mm2以上,較好為78 mm2以上,最好為300 mm2以上。氣體混合空間或反應氣 體經路為圓筒形配管時,其内徑設定為6 mm以上,較好為 10 mm以上,最好為20 mm以上。又,為抑制析出粉末引 起之閉塞,以便將氣體混合空間或反應氣體經路之反應速 99619.doc -15- 200535275 度保持在成膜室内之反應速度之50倍以下’在成膜室内之 麼力為200 Pa時,有必要將配管内壓力控制於⑽⑽ t〇rr)以下。此時,以配管内徑6 mm沉積厚1 之透明導電 膜時,可施行50批以上之成膜。 又’為了在即使在氣體混合空間或反應氣體經路閉塞時 也可容易加以掃除,最好在氣體混合空間及反應氣體經路 之至少-部分界設可却下及再安裝之接頭。作為接頭,最 好使用可充分施行真空密封而對有機金屬蒸氣與氧化劑基 氣具有化學的耐性之接頭。具體上,以使用金屬密封接 頭,例如密封材料使用不銹鋼之接頭為宜。又,以使用〇 f環接m密封材料使用含氟橡膠或鐵氣龍(註冊商 標)之接頭為宜。X ’ 〇型環接頭之—種之緊固接頭⑽ 可不必用工具,即可簡便卸下再安裝,故可容易施 行氣體混合空間或反應氣體經路之掃除。 又本^明之透明導電膜並不限定於氧化鋅膜。同樣 地,本發明也可適用於以有機金屬蒸氣與氧化劑蒸氣之低 垒…CVD可形成之其他透明導電膜。又,有機金屬蒸氣並 F疋於DEZ瘵氣。作為DEZ以外之有機金屬蒸氣之例, 口歹〗牛一甲基鋅蒸氣,但也可同樣使用可利用於形成透明 導電膜之其他有機金屬蒸氣。 本發明之氧化劑蒸氣並不限定於出0蒸氣。作為Η2〇以 外之氧化劑蒸氣之例,可列舉氧、二氧化碳、—氧化碳、 虱化一虱、二氧化氮、二氧化硫、五氧化二氮、醇類 ((〇Η))、_ 類(R(C0)R,)、醚類(ROR,)、醛類(r(COH))、 99619.doc -16- 200535275 3)、及亞砜類(R(SO)R,)等 胺類(RCO)x(NH3_x)、X=1 且同樣可使用可形錢明導電膜之有效之其他任意之氧化 劑蒸氣。又,在此R&amp;R,係表示烷基。 本發明之氣並不限定^A]•。作為㈣外之載氣之例, I使用其他稀有氣體(He、Ne、Kr、Xe、Rn)、氮、氯 等又肖樣可使用對有機金屬蒸氣及氧化劑蒸氣實質上 不具有活性之氣體。The temperature control of at least-part at least-part of the wall surface of the concrete working room and the reaction gas path is ~~ ⑽. c, It is preferably controlled to 50 ~ 8 (TC, and preferably controlled in the range of 55 to 6 generations. As the surface heater 13, for example, a resistance heating type heater (bell-mounted teaching device: belt heater) , Silicone rubber heater), infrared heater, heating medium circulation heater (heater that circulates heating oil or water and other fluids), etc. When the cross-sectional area of the gas mixing space or reaction gas path is small, the air flow mobility will change. Compared with the pressure in the film forming chamber, the pressure in the gas mixing space or the reaction gas path will become very high. At this time, when DEZ and HA are mixed in the gas mixing space, the film and powder are generated in the piping and the Occlusion occurs for a short time. In order to avoid occlusion of the piping, in the present invention, the cross-sectional area of the gas flow between the gas mixing space and the reaction gas path is set to 28 mm2 or more, preferably 78 mm2 or more, and most preferably 300 mm2 or more. Gas When the mixing space or the reaction gas path is a cylindrical pipe, its inner diameter is set to 6 mm or more, preferably 10 mm or more, and more preferably 20 mm or more. In order to suppress the blockage caused by the precipitated powder, the gas is blocked. Mixed space The reaction speed of the reaction gas path is 99,619.doc -15- 200535275 degrees, which is less than 50 times the reaction speed in the film forming chamber. When the force in the film forming chamber is 200 Pa, it is necessary to control the pressure in the pipe to ⑽⑽ t 〇rr) or less. At this time, when a transparent conductive film with a thickness of 1 is deposited with a pipe inner diameter of 6 mm, more than 50 batches of film can be formed. In addition, in order to be easily cleaned even when the gas mixing space or the reaction gas passage is blocked, it is preferable to provide a joint that can be lowered and reinstalled at least in a part of the boundary between the gas mixing space and the reaction gas passage. As the joint, it is preferable to use a joint capable of sufficiently performing vacuum sealing and having chemical resistance to organic metal vapor and oxidant base gas. Specifically, it is preferable to use a metal sealing joint, for example, a joint using stainless steel as a sealing material. In addition, it is preferable to use a joint of fluoro rubber or iron gas dragon (registered trademark) using o f ring joint m sealing material. X ’〇 ring joint—a kind of fastening joint⑽ It can be easily removed and reinstalled without using tools, so it is easy to clean the gas mixing space or the reaction gas path. The transparent conductive film is not limited to a zinc oxide film. Similarly, the present invention can also be applied to other transparent conductive films which can be formed by the low barrier of organic metal vapor and oxidant vapor ... CVD. In addition, the organometallic vapor is desorbed in the DEZ gas. As an example of an organometallic vapor other than DEZ, oxomethyl zinc vapor is used, but other organometallic vapors that can be used to form a transparent conductive film can be used in the same manner. The oxidant vapor of the present invention is not limited to 0 vapor. Examples of oxidant vapors other than Η20 include oxygen, carbon dioxide, carbon dioxide, lice, nitrogen dioxide, sulfur dioxide, dinitrogen pentoxide, alcohols ((〇Η)), _ (R ( C0) R,), ethers (ROR,), aldehydes (r (COH)), 99619.doc -16- 200535275 3), and amines (RCO) such as sulfoxides (R (SO) R,) x (NH3_x), X = 1 and the same can be used for any other oxidant vapor which is effective for the shape of Qianming conductive film. Here, R &amp; R represents an alkyl group. The spirit of the present invention is not limited to ^ A] •. As an example of a carrier gas other than tritium, I use other rare gases (He, Ne, Kr, Xe, Rn), nitrogen, chlorine, etc. In addition, a gas that is substantially inert to organometallic vapors and oxidant vapors can be used.

本發明之基體並不限定於玻躲板。作為玻璃基板以外 之基體之例’可使用金屬板、金制、有機膜等,只要可 耐成膜時之溫度且放出氣體少之材料皆可同樣使用。又, 基體不必為板本發明也可適詩具有曲面等之不定形 表面之基體。 作為基體之大小,本發明最好適用於可沉積之透明導電 膜之基體之表面區域面積在220 cm2以上,尤其是在13〇〇 cm以上之情形。在後述之比較例2及比較例*中,與基體 中央區域相比,具有95%以上之膜厚均勻性之區域分別只 能實現至約220 cm2與約1300 cm2。即,對大於此之成膜面 積之基體,不能均勻地製作透明導電膜。另一方面,在後 述之本發明之實施例1中,與基體中央區域相比,具有 95¾以上之膜厚均勻性之區域可擴大至約958〇 cm2。 為提高透明導電膜之導電率,除了有機金屬蒸氣與氧化 劑療氣以外,混合含有3族元素之氣體相當有效。而在適 用提高導電率之透明導電膜之裝置中,可降低電阻損耗。 作為含有3族元素之氣體,例如可使用含有乙硼院、三 99619.doc 200535275 基硼、二氟化鵬或三f基鋁等氣體。 為防止透明導電膜形成於基板之背 能中,使玻璁其4 ,在圖5之實施型 :觸於板面接觸於加熱器2。使基板之背面 =防=取代使基板之背面接觸於加熱器也可 ' 、於其背面。例如,使用熱傳導性良好之全屬 板或石反板作為其板狀構件時,在基板溫度之均句化,甚至 :基板上之透明導電膜之膜厚與物性之均勾化上亦甚理 想。The substrate of the present invention is not limited to glass hiding plates. Examples of substrates other than glass substrates include metal plates, gold, organic films, and the like, as long as they can withstand the temperature at the time of film formation and have low outgassing. In addition, the substrate need not be a substrate of the present invention, and may be a substrate having an irregular surface such as a curved surface. As the size of the substrate, the present invention is preferably applicable to the case where the surface area of the substrate of the transparent conductive film that can be deposited is 220 cm2 or more, especially 1300 cm or more. In Comparative Example 2 and Comparative Example * described later, compared with the central region of the substrate, regions having a film thickness uniformity of 95% or more can only be achieved to about 220 cm2 and about 1300 cm2, respectively. That is, a transparent conductive film cannot be uniformly formed on a substrate having a film formation area larger than this. On the other hand, in Example 1 of the present invention described later, compared with the central region of the substrate, a region having a film thickness uniformity of 95¾ or more can be enlarged to about 9580 cm2. In order to increase the conductivity of the transparent conductive film, in addition to organometal vapor and oxidant gas, it is quite effective to mix a gas containing a Group 3 element. In the device suitable for the transparent conductive film for improving the conductivity, the resistance loss can be reduced. As a gas containing a Group 3 element, for example, a gas containing diboron, tri-99619.doc 200535275-based boron, difluoride, or tri-f-based aluminum can be used. In order to prevent the transparent conductive film from being formed in the back surface of the substrate, the glass substrate 4 is used. In the embodiment shown in FIG. 5, the substrate 2 is in contact with the heater 2. Making the back surface of the substrate = prevent = instead of bringing the back surface of the substrate into contact with the heater may be used. For example, when using an all-metal plate or stone plate with good thermal conductivity as its plate-like member, the temperature of the substrate is uniform, and even: the thickness and physical properties of the transparent conductive film on the substrate are ideal. .

在圖5之實施型態中’作為基板之加熱手段,雖例示使 用:裝加熱器,但也可同樣使用鑄入型加熱器、紅外燈加 熱器、溫媒循環加熱器等。 圖15之模式的剖面圖係表示本發明之另一實施型態之光 電變換裝置。在此光電變換裝置之製作中,使用圖5之成 膜裝置,在玻璃基板16上形成氧化辞膜作為表面電極17。 在表面電極17上,以電漿CVD法形成含pin接合之第一薄 膜半導體光電變換單元18及同樣地含pin接合之第二薄膜 半導體光電變換單元19。在該第二單元19上,利用錢射法 形成金屬層作為背面電極20。在此光電變換裝置中,由玻 璃基板16側入射之光被構成混合型構造之第一光電變換單 元18與第二光電變換單元19施行光電變換。 第一光電變換單元1 8係由摻雜B (爛)之非晶質碳化石夕之 第一 p型半導體層18a、非晶質矽之第一真性半導體層 18b、及摻雜P(磷)之微晶矽之第一η型半導體層18c所構 成。第二光電變換單元19係由摻雜B之微晶石夕之第二p型半 99619.doc -18- 200535275 /導體層19a、多晶砍之第二真性半導體層⑽、及摻雜p之 Μ曰曰矽之第一 n型半導體層J 9c所構成。第二真性半導體層 使用多晶石夕之理由在於與非晶f石夕相,多晶石夕可吸收較 長波長之光,故未完全被第一真性半導體層18b吸收之長 波長之光可被第二真性半導體層19b吸收,而可提高光電 麦換裝置之隶大電力(Pmax)之故。In the embodiment shown in Fig. 5, as the heating means of the substrate, although a heater is used as an example, a cast-in heater, an infrared lamp heater, a heating medium circulation heater, etc. may be used in the same manner. Fig. 15 is a schematic sectional view showing a photovoltaic converter according to another embodiment of the present invention. In the production of this photoelectric conversion device, an oxide film is formed on the glass substrate 16 as the surface electrode 17 using the film forming device of FIG. 5. On the surface electrode 17, a first thin-film semiconductor photoelectric conversion unit 18 with a pin junction and a second thin-film semiconductor photoelectric conversion unit 19 with a pin junction are formed by a plasma CVD method. On the second unit 19, a metal layer is formed as the back electrode 20 by a coin shooting method. In this photoelectric conversion device, light incident from the glass substrate 16 side is subjected to photoelectric conversion by the first photoelectric conversion unit 18 and the second photoelectric conversion unit 19 which constitute a hybrid structure. The first photoelectric conversion unit 18 is composed of a first p-type semiconductor layer 18a doped with amorphous carbon carbide doped with B (rotten), a first true semiconductor layer 18b with amorphous silicon, and doped with P (phosphorus). It is composed of the first n-type semiconductor layer 18c of microcrystalline silicon. The second photoelectric conversion unit 19 is composed of a second p-type half of B-doped microcrystalline stone. 99619.doc -18- 200535275 / conductor layer 19a, a polycrystalline second true semiconductor layer ⑽, and a p-doped M is composed of the first n-type semiconductor layer J 9c of silicon. The reason for using the polycrystalline stone in the second true semiconductor layer is that the polycrystalline stone can absorb light with a longer wavelength than the amorphous phase. Therefore, the long wavelength light that is not completely absorbed by the first true semiconductor layer 18b can be used. It is absorbed by the second true semiconductor layer 19b, which can increase the Pmax of the photovoltaic device.

在表面電極17中’其厚度愈大時,丨薄膜電阻愈降低, 藉此’光電變換裝置之電阻損耗會變少…表面電極” 之厚度愈大時,其表面凹凸愈大,入射於光電變換裝置之 光“丈射而延長貫質的光程長,可增大光電變換裝置之短 路電流㈣。但’表面電極17太厚時,表面電極π之光吸 收損耗會擴大,Ise會減少。目此,㈣料面電㈣之透 明導電膜之厚度存在著適切之範圍,較好存在於 ㈣’更好存在於⑴_ ’最好存在於15至25㈣之範圍 内。 山在圖15之貫施型態中,第_ρ型半導體層心使用非晶質 石厌化石夕’但本發明並非限定於此。為使第—光電變換單元 18產生充分之擴散電位,也可使用摻雜b或Μ之非晶質矽 或寬帶隙之非晶質矽合金(非晶質碳化矽、非晶質氧化 石夕、非晶質氮化石夕)等。尤#,為減少第—p型半導體層 18a之光吸收損耗,最好使用寬帶隙之非晶質砍合金。作 為第-η型半導體層18c ’也可使用摻雜p之非晶質矽。 在圖15之實施㈣巾’真性半㈣層雖制非晶質石夕與 多晶矽,但亦可使用其他非單晶石夕系半導體之微晶石夕、非 99619.doc -19- 200535275 晶質石夕合金、微晶石夕合金、多晶石夕合金等。作為石夕合金, 例如最好使用錯、碳、氮、及氧之一種元素之石夕合金。 在圖15之實施型態中’在光電變換裝置雖使用矽系薄膜 • 帛導體,但亦可使用化合物半導體,例如銅銦砸、銅銦鎵 • 硒、硫化鎘、硫化碲等。 在圖15之實施型態之光電變換裝置中,雖依透明玻璃基 板、透明導電膜、半導體層及金屬層之順序疊層,但本發 明並非限定於此。例如,本發明也可適用於例如依不透明 • *屬基板、半導體層及透明導電膜之順序疊層之光電變換 裝置。又,光電變換裝置所含之光電變換單元並非如圖15 所示限定於2段疊層之光電變換單元,本發明也可適用於 含1段以上之任意段數光電變換單元之光電變換裝置。 圖19之杈式的剖面圖係表示本發明之又另一實施例之大 面積薄膜光電變換裝置。大面積薄膜光電變換裝置具有將 劃分成小面積之光電變換胞多數個互相串聯連接於玻璃基 板上之積體型光電變換模組之構造。各光電變換胞係利用 圖5之成膜裝置逐次施行形成於玻璃基板上之透明導電膜 之表面電極、疊層1個以上之薄膜半導體光電變換單元之 半導體部、及背面電極層之成膜與圖案化所形成。 圖19之積體型薄膜光電變換模組1〇1係在玻璃基板1〇2上 逐次疊層透明導電膜之表面電極層1〇3、含非晶質矽之真 性半導體層之pin接合構成之第一光電變換單元1〇4a、含 晶質矽之真性半導體層之pin接合構成之第二光電變換單 元104b、及背面電極層1〇6之構造。 99619.doc -20- 200535275 如圖19所示,在積體型薄膜光電變換模組ι〇1設有第1與 第2分離溝121、122及連接溝123。第1與第2分離溝121、 1 22及連接溝123互相平行,向垂直於圖式紙面之方向延 伸。又,一個光電變換胞110之發電區域係第丨與第2分離 溝121、122間之區域。 第1分離溝121係分別對應於光電變換胞11〇而分割表面 電極層103。即,第1分離溝121係將相鄰之表面電極層1〇3 彼此電性分離。同樣地,第2分離溝122係分別對應於光電 變換胞11〇而分割第一光電變換單元104a、第二光電變換 單兀104b、及背面電極層1〇6。即,第2分離溝122係在相 鄰之光電變換胞110間將背面電極層1〇6彼此電性分離。 連接溝123係設於第丨分離溝121與第2分離溝122之間, 用於分割第一光電變換單元1〇4a及第二光電變換單元 l〇4b。此連接溝123被埋入構成背面電極層1〇6之金屬材 料’用於將相鄰之光電變換胞11〇之一方背面電極層1〇6與 他方胞之表面電極層103電性串聯連接。即,連接溝丨23及 埋入該溝之金屬材料可使並置於玻璃基板1〇2上之光電變 換胞110彼此電性串聯連接。 在如此形成之積體型薄膜光電變換模組中’由於將小面 積之光電變換胞串聯連接,故該模組之發電電流會受到發 電電流最小之光電變換胞所限定。因此,為使一個模組所 含之多數胞之發電電流均勻化,利用圖5之成膜裝置形成 膜厚分布均勾之透明導電膜之表面電極層特別重要。 利用圖5之成膜裝置形成之透明導電膜之氧化辞膜也可 99619.doc 200535275 在光電變換裝置之半導體層與背 曰月面電極層間使用作為背面 反射層。該背面反射層太薄日夺,反射性不充分,太厚時, 該背面反射層之吸收損耗會增大,故其厚度有適::範 圍。作為光電變換裝置之半導體層,使用非晶質石夕或晶質 石夕,背面電極層使用金屬層,作為半導體層與金屬層間之 背面反射層,使用氧化鋅之透明導 π守电膜日守,该背面反射層 之厚度較好在10至150 nm、更好在305 又野在30至120 nm、最好在6〇 至90 run之範圍内。In the surface electrode 17, 'the larger the thickness, the lower the sheet resistance, thereby the' resistance loss of the photoelectric conversion device will be reduced ... the larger the thickness of the surface electrode ', the larger the surface unevenness, and incident on the photoelectric conversion The light of the device is "radiated" to extend the length of the optical path, which can increase the short-circuit current of the photoelectric conversion device. However, when the 'surface electrode 17 is too thick, the light absorption loss of the surface electrode π will increase and Ise will decrease. For this reason, the thickness of the transparent conductive film on the material surface exists in a suitable range, preferably ㈣ ′, more preferably ⑴_ ′, and most preferably 15 to 25 ㈣. In the embodiment shown in FIG. 15, the amorphous silicon anionite fossil is used as the core of the p-type semiconductor layer, but the present invention is not limited to this. In order to generate a sufficient diffusion potential for the first photoelectric conversion unit 18, b or M doped amorphous silicon or a wide band gap amorphous silicon alloy (amorphous silicon carbide, amorphous oxide, Amorphous nitride nitride eve) and so on. In particular, in order to reduce the light absorption loss of the p-type semiconductor layer 18a, it is preferable to use an amorphous chopped alloy with a wide band gap. As the -n-type semiconductor layer 18c ', p-doped amorphous silicon can also be used. In the implementation shown in FIG. 15, although the true semi-sacral layer is made of amorphous stone and polycrystalline silicon, microcrystalline stones of other non-single crystal semiconductors can also be used. Non-99619.doc -19- 200535275 crystalline Shi Xi alloy, microcrystalline Shi Xi alloy, polycrystalline Shi Xi alloy, etc. As the shixi alloy, for example, a shixi alloy that is one of the elements of carbon, nitrogen, and oxygen is preferably used. In the embodiment shown in FIG. 15, although a silicon-based thin film • rhenium conductor is used in the photoelectric conversion device, a compound semiconductor such as copper indium, copper indium gallium, selenium, cadmium sulfide, and tellurium sulfide can also be used. In the photoelectric conversion device of the embodiment shown in Fig. 15, although a transparent glass substrate, a transparent conductive film, a semiconductor layer, and a metal layer are laminated in this order, the present invention is not limited to this. For example, the present invention is also applicable to, for example, a photoelectric conversion device that is laminated in the order of an opaque substrate, a semiconductor layer, and a transparent conductive film. In addition, the photoelectric conversion unit included in the photoelectric conversion device is not limited to a two-layer laminated photoelectric conversion unit as shown in FIG. 15, and the present invention can also be applied to a photoelectric conversion device including an arbitrary number of photoelectric conversion units of one or more stages. Fig. 19 is a cross-sectional view showing a large-area thin-film photoelectric conversion device according to still another embodiment of the present invention. The large-area thin-film photoelectric conversion device has a structure of an integrated photoelectric conversion module in which a plurality of photoelectric conversion cells divided into a small area are connected in series to each other on a glass substrate. Each photoelectric conversion cell line uses the film-forming device of FIG. 5 to sequentially execute the surface electrode of a transparent conductive film formed on a glass substrate, the semiconductor portion of one or more thin-film semiconductor photoelectric conversion units laminated, and the film formation of the back electrode layer. Formed by. The integrated thin-film photoelectric conversion module 1001 of FIG. 19 is a pin-bonded structure consisting of a surface electrode layer 103 of a transparent conductive film and a true semiconductor layer containing amorphous silicon, which are successively laminated on a glass substrate 102. The structure of a photoelectric conversion unit 104a, a second photoelectric conversion unit 104b formed by pin bonding of a true semiconductor layer containing crystalline silicon, and a back electrode layer 106. 99619.doc -20- 200535275 As shown in FIG. 19, the integrated thin-film photoelectric conversion module ι01 is provided with first and second separation grooves 121 and 122 and a connection groove 123. The first and second separation grooves 121, 122, and the connection groove 123 are parallel to each other and extend in a direction perpendicular to the drawing surface. In addition, the power generation region of one photoelectric conversion cell 110 is a region between the first and second separation trenches 121 and 122. The first separation grooves 121 divide the surface electrode layer 103 in correspondence with the photoelectric conversion cells 110, respectively. That is, the first separation trench 121 electrically separates adjacent surface electrode layers 103 from each other. Similarly, the second separation trench 122 is divided into a first photoelectric conversion unit 104a, a second photoelectric conversion unit 104b, and a back electrode layer 106 corresponding to the photoelectric conversion cells 110 respectively. That is, the second separation trench 122 electrically separates the back electrode layers 106 from each other between adjacent photoelectric conversion cells 110. The connection groove 123 is provided between the first separation groove 121 and the second separation groove 122, and is used to divide the first photoelectric conversion unit 104a and the second photoelectric conversion unit 104b. This connection groove 123 is embedded in a metal material composing the back electrode layer 106 for electrically connecting the back electrode layer 106 of one of the adjacent photoelectric conversion cells 110 and the surface electrode layer 103 of the other cell in series. That is, the connection trench 23 and the metal material embedded in the trench can electrically connect the photoelectric conversion cells 110 placed on the glass substrate 102 in series with each other. In the integrated thin-film photoelectric conversion module thus formed ', since the small-area photoelectric conversion cells are connected in series, the power generation current of the module is limited by the photoelectric conversion cell having the smallest current generation. Therefore, in order to make the power generation current of the majority of cells contained in a module uniform, it is particularly important to form a surface electrode layer of a transparent conductive film with a uniform film thickness distribution using the film forming apparatus of FIG. 5. The oxide film of the transparent conductive film formed by the film forming apparatus of FIG. 5 can also be used as a back surface reflective layer between the semiconductor layer and the back surface electrode layer of the photoelectric conversion device. The back surface reflection layer is too thin, and the reflectivity is not sufficient. When the back surface reflection layer is too thick, the absorption loss of the back surface reflection layer will increase, so its thickness is suitable. As the semiconductor layer of the photoelectric conversion device, an amorphous stone or a crystalline stone is used, a metal layer is used for the back electrode layer, and a transparent conductive film of zinc oxide is used as the back reflective layer between the semiconductor layer and the metal layer. The thickness of the back reflective layer is preferably in the range of 10 to 150 nm, more preferably in the range of 305 to 30 to 120 nm, and most preferably in the range of 60 to 90 run.

利用圖5之成膜裝置形成之透明導電臈之氧化辞膜也可 使用作為含多數段之光電變換單元之串聯型光電變換裝置 中之中間層。例如可在圖15之光電變換裝置之第_光電變 換單元18與第二光電變換單元19之間,將透明導電膜之氧 化鋅膜設置作為中間層。該種中間層太薄日寺,光反射性及 光散射性不充分’太厚時,料間層之吸收損耗會增大, 故有理想之厚度範圍存在。第一光電變換單元此真性半 導體層18b使用非晶質石夕’中間層使用氧化辞膜,而第二 光電變換單元之真性半導體層19b使用多晶質矽時,該 中間層之厚度較好在2至150 nm、更好在1〇至1〇〇 nm、最 好在30至60nm之範圍内。 在圖15之實施型態中,雖為2個pin接合重疊,但本發明 當然也可適用於含1個以上之pin接合、nip接合、pn接合、 或np接合之光電變換裝置。 [實施例] 以下,與比較例同時詳細說明本發明之實施例。 99619.doc -22- 200535275 (比較例1) 在圖1之概念圖中,係作為比較例1,表示使用低壓熱 CVD之以往之透明導電膜之成膜裝置之一例。在此成膜裝 置中,真空槽4之内部為設置基板丨之成膜室3。作為含鋅 之有機金屬蒸氣,將二乙基鋅(DEZ)蒸氣在與^載氣混合 之狀態通過DEZ供應管7供應至成膜室3内。又,在比較例 U中,使用蒸發氣化器。DEZ供應管7係外徑1/4吋(内徑 約4.4 mm)之不銹鋼製管。為提高DEZ蒸氣之蒸氣壓以防 止液化,DEZ供應管7之一部分以加熱器71加熱至約8〇。〇。 虱化劑蒸氣之水(HA)蒸氣也在與Ar載氣混合之狀態通過 H2〇供應官8供應至成膜室3。Η&quot;供應管8亦係外徑1/4吋 (内徑約4.4 mm)之不銹鋼製管。為提高私〇蒸氣之蒸氣壓以防 止液化,H2〇供應管8之一部分以加熱器8丨加熱至約⑽它。 玻璃基板1被加熱器2加熱以施行低壓熱CVD,在玻璃基 板面1之表面沉積氧化鋅膜作為透明導電膜。作為加熱器2 為鎧裝加熱器。廢氣經由排氣口 5及排氣管6而被泵(未圖 不)排出。且可利用未表示於圖丨之電容壓力計與電容可變 閥將真空槽4中之壓力保持於一定。沉積氧化鋅膜時, 例如可設定為··真空槽4内之壓力1〇〇 Pa、基板溫度2〇(Γ(:、 DEZ蒸氣流量500 seem、H2〇蒸氣流量5〇〇 sccm,而^流 里DEZ供應管7與H20供應管相加為2000 sccm 0 (比較例2) 圖2之概略的平面圖係作為比較例2,以圖丨之成膜裝置 在1 mxl m之玻璃基板1形成氧化辞膜時之厚度分布。圖2中 99619.doc -23- 200535275 之數值係以^^單位表示膜厚之等高線。又,透明導電膜 之厚度係利用測定玻璃基板上之透明導電膜之反射率之波 長依存性,由干涉引起之反射率之變化求出膜厚。此測定 與分析係利用仙提克儀器公司製之晶圓製圖系統。 由圖1與圖2可知··在相當於DEZ供應管7與私〇供應管8 ^下方之部分,膜厚較大,向周緣移位時,膜厚急遽減 &gt;。又,在基板之周緣部分,完全無膜沉積。與基板中央 區域之膜厚相比,75%以上之膜厚區域,為基板面積之 5·8%之580 cm2’ |有95%以上之膜厚區域僅為基板面積之 2.2%之220 cm2。因此,DEZ與h2〇之反應僅在dez供應管 7與HA供應管8正下方附近進行而使膜厚分布變得極端不 良。在此比較例2十,由於在基板之周緣部分有完全無膜 沉積之區域存在,故透明導電膜不能適用於大面積之光電 變換裝置之表面電極。 (比較例3) 圖3之概念圖係作為比較例3,表示使用低壓熱cVD之以 往之透明導電膜之成膜裝置之另一例。與圖丨之比較例(同 樣地,在圖3中,真空槽4之内部也為成膜室3,玻璃基板i 可被加熱器2加熱。但在圖3中,〇ΕΖ與Ar之混合氣體係由 DEZ供應官7暫且進入擴散箱9内,由噴淋板丨〇之孔以喷淋 狀被供應至成膜室3。DEZ供應管7係外徑1 /4叫~(内徑約4 ·4 mm)之不錢鋼製管,DEZ供應管7之一部分以加熱器71加熱 至約80°C。HW與Ar之混合氣體係由在真空槽4之相向壁 面相向配置之2個Ηβ供應管8供應至成膜室3。H20供應管 99619.doc -24- 200535275 8亦係外徑1/4对(内徑約4.4 mm)之不銹鋼製管。h2〇供應 管8之一部分也被加熱器81加熱至約8(rc。玻璃基板丨被加 熱器2加熱而被施行低壓熱CVD ’在玻璃基板丨表面沉積透 明導電膜之氧化鋅膜。又,在此比較例3中,沉積氧化鋅 膜日守之氣體Μ力及氣體流量與比較例1之情形同。 (比較例4) 圖4之概略的平面圖係作為比較例4,以圖3之成膜裝置 在1 mxl m之玻璃基板1形成氧化鋅膜時之厚度分布。圖4 中之數值係以μηι單位表示膜厚之等高線。將此圖4之比較 例4與圖2之比較例2相比時,在玻璃基板沉積透明導電膜 之區域較寬。但在圖4之情形,也依然在基板中央區域中 透明導電膜之厚度較大,隨著向基板周緣移動,其膜厚逐 漸變薄。且膜厚較大之區域之中心偏向基板之約略右側, 可知在接近於圖3中之排氣口 5側膜厚變大。此係由於氣流 向排氣方向偏向基板1之右側之故。與基板中央區域之膜 厚相比,75%以上之膜厚區域,為基板面積之386%之 3860 cm2,具有95%以上之膜厚區域為基板面積之13」%之 13 10 cm。如後述之比較例6所示,此透明導電膜適用於 大面積之光電變換裝置之表面電極時,只能獲得極低之光 電變換特性,該膜並未具有可適用於大面積裝置之充分均 勻之膜厚分布。 (比較例5) 在比較例5中,係在圖3之成膜裝置中,將混合DE墓 &gt;、、、 氣、HA蒸氣與Ar之反應氣體供應至βΕζ供應管7。此情 99619.doc -25- 200535275 形’ DEZ供應管7約在1〜2分鐘就會被析出粉體所閉塞,無 法在基板1上形成透明導電膜。此時,在成膜室3之壓力約 100 Pa之情形’將DEZ與Ar之合計流量設定為1〇00 sccm 時,DEZ供應管7中之壓力約達5000 Pa。The oxide film of the transparent conductive rhenium formed by the film-forming device of Fig. 5 can also be used as an intermediate layer in a tandem-type photoelectric conversion device having a plurality of photoelectric conversion units. For example, a zinc oxide film of a transparent conductive film may be provided as an intermediate layer between the _th photoelectric conversion unit 18 and the second photoelectric conversion unit 19 of the photoelectric conversion device of FIG. 15. This kind of intermediate layer is too thin. If the light reflectivity and light scattering properties are not sufficient, the absorption loss of the material layer will increase, so there exists a desirable thickness range. When the true semiconductor layer 18b of the first photoelectric conversion unit uses amorphous silicon, the intermediate layer uses an oxide film, and when the true semiconductor layer 19b of the second photoelectric conversion unit uses polycrystalline silicon, the thickness of the intermediate layer is preferably at 2 to 150 nm, more preferably 10 to 100 nm, and most preferably 30 to 60 nm. In the embodiment shown in Fig. 15, although two pin junctions are overlapped, the present invention is of course applicable to a photoelectric conversion device including more than one pin junction, nip junction, pn junction, or np junction. [Examples] Hereinafter, examples of the present invention will be described in detail together with comparative examples. 99619.doc -22- 200535275 (Comparative Example 1) In the conceptual diagram of Fig. 1, as Comparative Example 1, an example of a conventional film forming apparatus for a transparent conductive film using low-pressure thermal CVD is shown. In this film forming apparatus, the inside of the vacuum chamber 4 is a film forming chamber 3 on which a substrate 丨 is provided. As the zinc-containing organometal vapor, diethylzinc (DEZ) vapor is supplied to the film forming chamber 3 through a DEZ supply pipe 7 in a state of being mixed with a carrier gas. In Comparative Example U, an evaporative gasifier was used. The DEZ supply pipe 7 is a stainless steel pipe with an outer diameter of 1/4 inch (inner diameter of about 4.4 mm). In order to increase the vapor pressure of the DEZ vapor to prevent liquefaction, a part of the DEZ supply pipe 7 is heated by a heater 71 to about 80. 〇. Water (HA) vapor of lice agent vapor is also supplied to the film forming chamber 3 through the H2O supply unit 8 in a state of being mixed with the Ar carrier gas.供应 &quot; Supply tube 8 is also a stainless steel tube with an outer diameter of 1/4 inch (inner diameter of about 4.4 mm). In order to increase the vapor pressure of the private steam to prevent liquefaction, a part of the H2O supply pipe 8 is heated to about ⑽ with a heater 8. The glass substrate 1 is heated by the heater 2 to perform low-pressure thermal CVD, and a zinc oxide film is deposited on the surface of the glass substrate surface 1 as a transparent conductive film. As heater 2 is an armored heater. The exhaust gas is discharged by a pump (not shown) through an exhaust port 5 and an exhaust pipe 6. The capacitance pressure gauge and the variable capacitance valve not shown in the figure can be used to keep the pressure in the vacuum tank 4 constant. When depositing a zinc oxide film, for example, the pressure in the vacuum tank 4 can be set to 100 Pa, the substrate temperature can be 20 ° (Γ (:, DEZ vapor flow rate 500 seem, H2O vapor flow rate 500 seem), and Here, the DEZ supply pipe 7 and the H20 supply pipe are added to 2000 sccm 0 (Comparative Example 2). The schematic plan view of FIG. 2 is used as Comparative Example 2, and the film forming apparatus of FIG. Thickness distribution at the time of film. The value of 99619.doc -23- 200535275 in Figure 2 represents the contour line of the film thickness in ^^ units. In addition, the thickness of the transparent conductive film is determined by measuring the reflectance of the transparent conductive film on the glass substrate. The thickness of the film is determined by the change in reflectance caused by interference. This measurement and analysis is performed using a wafer mapping system made by Sendek Instruments. As shown in Figures 1 and 2, it is equivalent to a DEZ supply tube. 7 and the private 0 supply tube 8 ^ The film thickness is large, and the film thickness decreases sharply when shifted to the periphery. Also, there is no film deposition at the peripheral portion of the substrate. It is in accordance with the film thickness in the central area of the substrate. Ratio, more than 75% of the film thickness area, 580% of the substrate area of 5.8% cm2 '| more than 95% of the film thickness area is only 2.2% of the substrate area of 220 cm2. Therefore, the reaction between DEZ and h2〇 is only carried out near the directly below the dez supply pipe 7 and HA supply pipe 8 to make the film thickness distribution It becomes extremely bad. In Comparative Example 20, since there is a completely non-film-deposited area on the peripheral edge of the substrate, the transparent conductive film cannot be applied to the surface electrode of a large-area photoelectric conversion device. (Comparative Example 3) Figure The conceptual diagram 3 is another comparative example 3, showing another example of a conventional film-forming apparatus using a low-voltage thermal cVD. Similar to the comparative example in FIG. 丨 (Similarly, in FIG. 3, the inside of the vacuum tank 4 is also For the film forming chamber 3, the glass substrate i can be heated by the heater 2. However, in FIG. 3, the mixed gas system of OEZ and Ar is temporarily supplied into the diffusion box 9 by the DEZ supply officer 7, and the hole of the shower plate It is supplied to the film-forming chamber 3 in a spray shape. The DEZ supply pipe 7 is a stainless steel pipe with an outer diameter of 1/4 called ~ (inner diameter of about 4 · 4 mm). Part of the DEZ supply pipe 7 is a heater 71. It is heated to about 80 ° C. The mixed gas system of HW and Ar is supplied by two Ηβ arranged opposite to each other on the opposite wall surface of the vacuum tank 4. The supply pipe 8 is supplied to the film forming chamber 3. The H20 supply pipe 99619.doc -24- 200535275 8 is also a stainless steel pipe with an outer diameter of 1/4 pair (inner diameter of about 4.4 mm). A part of the h20 supply pipe 8 is also The heater 81 is heated to about 8 (rc.) The glass substrate 丨 is heated by the heater 2 and subjected to low-pressure thermal CVD. A transparent conductive film of zinc oxide is deposited on the surface of the glass substrate 丨. In this comparative example 3, oxide was deposited. The gas force and gas flow rate of the zinc film daily guard were the same as those in Comparative Example 1. (Comparative Example 4) The schematic plan view of Fig. 4 is Comparative Example 4, and the thickness distribution when the zinc oxide film was formed on the 1 mxl m glass substrate 1 by the film forming apparatus of Fig. 3 was used. The numerical values in FIG. 4 represent contour lines of film thickness in μm units. Comparing this comparative example 4 of FIG. 4 with the comparative example 2 of FIG. 2, the area where the transparent conductive film is deposited on the glass substrate is wider. However, in the case of Fig. 4, the thickness of the transparent conductive film is still large in the central region of the substrate, and the film thickness gradually becomes thinner as it moves toward the periphery of the substrate. And the center of the region with a larger film thickness is shifted to the slightly right side of the substrate, and it can be seen that the film thickness becomes larger near the exhaust port 5 side in FIG. 3. This is because the airflow is deviated to the right side of the substrate 1 in the exhaust direction. Compared with the film thickness in the central area of the substrate, a film thickness area of more than 75% is 3860 cm2 of 386% of the substrate area, and a film thickness area of 95% or more is 13 10% of the substrate area. As shown in Comparative Example 6 described later, when this transparent conductive film is applied to a surface electrode of a large-area photoelectric conversion device, only a very low photoelectric conversion characteristic can be obtained, and the film does not have sufficient uniformity suitable for a large-area device. Film thickness distribution. (Comparative Example 5) In Comparative Example 5, in the film-forming apparatus of Fig. 3, a reaction gas of mixed DE grave gas, HA gas, HA vapor, and Ar was supplied to the βEζ supply pipe 7. In this case, 99619.doc -25- 200535275 The shape of the DEZ supply pipe 7 is blocked by the precipitated powder in about 1 to 2 minutes, and a transparent conductive film cannot be formed on the substrate 1. At this time, when the pressure of the film forming chamber 3 is about 100 Pa ', when the total flow rate of DEZ and Ar is set to 10,000 sccm, the pressure in the DEZ supply pipe 7 reaches about 5000 Pa.

原料氣體被充分供應時,DEZ與H2〇之反應速度係和 DEZ洛氣與出0療氣之各分壓成正比,故其反應速度與全 壓力之2次方成正比。在此比較例5之情形,氣體混合空間 内之壓力係成膜室内之壓力之5〇倍,故在氣體混合空間 内,與成膜室内相比,以2500倍之速度進行反應,故在配 官内產生透明導電膜或粉體而發生閉塞。且由於管内徑小 至約4.4 mm,隨著粉體之形成,氣體通路逐漸變細,壓力 愈來愈大,反應近一步進行時,在短時間配管就會閉塞。 另外,在比較例5中,由於使用蒸氣氣化器,同樣溫度 下’ DEZ蒸氣壓低於h2〇蒸氣壓,Μζ蒸氣與h2〇蒸氣無法 密切混合。而,仔細觀察閉塞之配管時,發現mz接近於 氣化器測之配管之閉塞比Η&quot;接近於氣化器測之配管嚴 重,因此,認為DEZ蒸氣有被Η&quot;蒸氣推回來之傾向。 (實施例1) 使用圖5之成臈裝置形成氧化鋅 作為本發明之實施例 膜。在此實施例1中,佶用缸、、由名儿— 使用起/包乳化态,氣體混合空間12 及反應氣體經路之壁面溫度被控制於6(rc。又,在實施例 1使用之圖21之配管之距離皆為〇15 m。反應氣配管 U使用大於以往之内徑約25醜之圓筒管,其—部分被 NW25型緊固接頭(未圖示)所連接。由於其管徑充分大, 99619.doc -26- 200535275 故氣流導通性增大,氣體混合空間12及反應氣體經路之壓 力變小,故可抑制管之閉塞。且只要卸下緊固接頭,即可 容易地施行管内之粉體或透明導電膜之掃除。使用實施例 1之成膜裝置之結果’在成膜室3内之慶力1 〇〇 pa、氣體混 合空間内之壓力300 Pa下,即使施行總共3〇〇小時以上之 成膜,配管也不會閉塞。即,實施例丨可說是工業上可充 分使用之成膜方法。 (實施例2) 圖6之概略的平面圖係作為實施例2,以圖$之成臈裝置 在1 mx 1 m之玻璃基板1形成氧化鋅膜時之厚度分布。在 1 mxl m之玻璃基板1形成氧化鋅膜時,喷淋板⑺之大小以 例如1.1 mxl.l m較為適當。又,在成膜時,成膜室3内之 壓力為100 Pa、基板溫度為20(rc、DEZ蒸氣流量為5〇() seem、H20蒸氣流量為50〇 sccm,而^流量為2〇〇〇 sccm。 圖6中之數值係以/^111單位表示膜厚之等高線。除基板之 四角之區域外,可獲得均勻之膜厚分布。圖5之成膜裝置 之右側有排氣口 5,與基板之四角中接近於排氣口 5之右側 之二角相比,在較遠之左側之二角中膜厚較小之區域稍 寬。與基板中央區域之膜厚相比,75%以上之膜厚區域為 基板面積之98.6%之9860 cm2,具有95%以上之膜厚區域為 基板面積之95.8%之9580 cm2。因此,在實施例2中,可知 膜厚之均勻性與比較例2及4獲得顯著之改善。 另外,调查透明導電膜之特性之結果,適合於光電變換 I置之80%以上之透光率(波長4〇〇 nm〜1〇〇〇 nm)、ΐ5Ω/〇 99619.doc -27- 200535275 以下之薄膜電阻及1 〇%以上之光霧率之特性可在成膜室壓 力為5〜200 Pa之範圍内獲得。且在此範圍内之成膜室壓力 中,可獲得厚度方向1 nm/s以上之快的成膜速度。又,所 謂光霧率,係以光學方式評估透明之基板之表面凹凸之指 標,以(擴散透過率/全光線透過率)χ1〇〇[%]表示(JIS K7136) 〇 成膜至&gt;£力低於5 Pa時’成膜速度會低於1 nm/s,透明 導電膜之成膜時間會延長,製造成本會升高。又,為降低 成膜室壓力,需要高排氣能力之泵,故製造成本會升高。 另一方面,成膜室壓力高於200 Pa時,無法獲得適合於 如上述之光電變換裝置之特性。又,成膜室壓力在2〇〇 pa 以下日守’在氣體混合空間之内徑25 mm之情形,該氣體混 合空間内之壓力在3〇〇 pa以下不受成膜室壓力影響而大致 保持疋’但若成膜室壓力高於200 Pa時,氣體混合空間 内之壓力即會顯著地與成膜室壓力成正比地顯著升高。而 成膜至壓力南於200 Pa時,配管容易閉塞。 (實施例3) 圖7之概念圖係表示實施例3之成膜裝置。與圖5之成膜 裝置相比,此圖7之成膜裝置係僅在加熱器2之中央下方配 置排氣口 5與排氣管6之部分相異。將排氣口 5配置在加熱 器2之中央下方,可使由成膜室3排出之氣流對稱地接近基 板1之中央。又,在本實施例3以後之實施例中,使用噴霧 氣化器。 (實施例4) 99619.doc -28- 200535275 圖8之概略的平面圖係料實施例4,以圖7之成膜裝置 ^ 阳之玻璃基板1形成氧化鋅膜時之厚度分布。在此 :加例4 t ’在形成氧化辞膜時,氣體遷力及氣體流量與 员施例2之情形相同。圖$中皇 τ之數值係以早位表示膜厚 之等高,。將圖8與圖6作比較日寺,可知:與實施例”目 比’在貫施例4中,可推一 〇Κ ¥ π+. _ J進 V改善Μ厚均勻性。在圖8中, 基板四角之臈厚較薄區域之大小在基板之左側與右側大致When the raw material gas is fully supplied, the reaction speed of DEZ and H2O is proportional to the partial pressures of DEZ and gas, and therefore the reaction speed is proportional to the second power of the full pressure. In the case of Comparative Example 5, the pressure in the gas mixing space is 50 times the pressure in the film forming chamber. Therefore, in the gas mixing space, the reaction proceeds at a speed of 2500 times compared to the film forming chamber. Occurrence of occlusion due to transparent conductive film or powder inside the body. And because the inner diameter of the tube is as small as about 4.4 mm, as the powder is formed, the gas path becomes gradually narrower, and the pressure becomes larger and larger. When the reaction proceeds in a short period, the piping will be blocked in a short time. In Comparative Example 5, since a vaporizer was used, the 'DEZ vapor pressure was lower than the h20 vapor pressure at the same temperature, and the Mζ vapor and the h20 vapor could not be closely mixed. However, when observing the closed piping carefully, it was found that the mz is close to the piping measured by the gasifier, and "close to the piping measured by the gasifier." Therefore, it is believed that the DEZ vapor has a tendency to be pushed back by the Η &quot; vapor. (Example 1) Zinc oxide was formed as a film according to the present invention using the hafnium-forming apparatus of Fig. 5. In the first embodiment, the cylinders, and the faucets are used in an emulsified state, and the wall temperatures of the gas mixing space 12 and the reaction gas passage are controlled to 6 (rc. In addition, in the first embodiment, The distance between the piping in Figure 21 is 015 m. The reaction gas piping U uses a cylindrical tube with an inner diameter of about 25 ugly larger than that in the past, and its-part is connected by NW25 type fastening joint (not shown). The diameter is sufficiently large, 99619.doc -26- 200535275, so the airflow conductivity is increased, the pressure of the gas mixing space 12 and the reaction gas path is reduced, so that the occlusion of the tube can be suppressed. And as long as the fastening joint is removed, it can be easily The powder or transparent conductive film in the tube is cleaned on the ground. The result of using the film-forming device of Example 1 is' 100 Pa in the film-forming chamber 3 and pressure 300 Pa in the gas mixing space, even if it is performed. For a total of more than 300 hours of film formation, the piping will not be blocked. That is, Example 丨 can be said to be a film forming method that can be used industrially. (Example 2) The schematic plan view of FIG. 6 is Example 2. In the figure, the device is formed on a glass substrate 1 of 1 mx 1 m. Thickness distribution when the zinc film is formed. When a zinc oxide film is formed on a glass substrate 1 of 1 mxl m, the size of the shower plate 以 is, for example, 1.1 mxl.lm. Also, during film formation, The pressure is 100 Pa, the substrate temperature is 20 (rc, the DEZ vapor flow rate is 50 °), the H20 vapor flow rate is 50 sccm, and the flow rate is 2000 sccm. The values in FIG. 6 are expressed as / ^ 111 The unit indicates the contour line of the film thickness. Except for the four corners of the substrate, a uniform film thickness distribution can be obtained. The right side of the film forming device in Fig. 5 has an exhaust port 5, which is close to the right side of the exhaust port 5 in the four corners of the substrate Compared with the two corners, the area with a smaller film thickness is slightly wider in the two corners on the far left side. Compared with the film thickness in the center area of the substrate, more than 75% of the film thickness area is 98.6% to 9860 cm2 of the substrate area. The area with a film thickness of 95% or more is 95.8% of 9580 cm2 of the substrate area. Therefore, in Example 2, it can be seen that the uniformity of the film thickness is significantly improved as compared with Comparative Examples 2 and 4. In addition, the transparent conductive film was investigated. As a result of the characteristics, it is suitable for a light transmittance of more than 80% (wavelength of 400 n). m ~ 100nm), ΐ5Ω / 〇99619.doc -27- 200535275, the characteristics of sheet resistance below 1035275 and haze rate above 10% can be obtained in the range of 5 ~ 200 Pa of film forming chamber pressure. And in the pressure of the film forming chamber within this range, a fast film forming speed of 1 nm / s or more in the thickness direction can be obtained. Also, the so-called haze rate is an index for optically evaluating the surface unevenness of a transparent substrate, (Diffusion transmittance / total light transmittance) χ 100 (%) (JIS K7136) 〇 Film formation to &gt; When the force is lower than 5 Pa, the film formation speed will be lower than 1 nm / s. Film formation time will be prolonged, and manufacturing costs will increase. In addition, in order to reduce the pressure of the film forming chamber, a pump having a high exhausting capacity is required, so the manufacturing cost will increase. On the other hand, when the pressure of the film forming chamber is higher than 200 Pa, characteristics suitable for the photoelectric conversion device as described above cannot be obtained. In addition, when the pressure of the film forming chamber is less than 2000 Pa, when the inner diameter of the gas mixing space is 25 mm, the pressure in the gas mixing space is less than 300 Pa. It is generally maintained regardless of the pressure of the film forming chamber.疋 'However, if the pressure of the film forming chamber is higher than 200 Pa, the pressure in the gas mixing space will significantly increase in proportion to the pressure of the film forming chamber. When the film is formed to a pressure of 200 Pa, the piping is easily blocked. (Embodiment 3) The conceptual diagram of FIG. 7 shows a film forming apparatus of Embodiment 3. Compared with the film-forming apparatus of FIG. 5, the film-forming apparatus of FIG. 7 is different only in that the exhaust port 5 and the exhaust pipe 6 are arranged below the center of the heater 2. The exhaust port 5 is arranged below the center of the heater 2, so that the airflow discharged from the film forming chamber 3 can approach the center of the substrate 1 symmetrically. It should be noted that, in Examples 3 and later, a spray vaporizer is used. (Embodiment 4) 99619.doc -28- 200535275 The schematic plan view of FIG. 8 is based on Embodiment 4, and the thickness distribution when the zinc oxide film is formed on the glass substrate 1 of FIG. Here: Addition Example 4 t ′ When forming the oxide film, the gas migration force and the gas flow rate are the same as those in Example 2. In the figure, the value of the emperor τ represents the height of the film thickness in the early position. Comparing FIG. 8 with FIG. 6, it can be seen that, in the fourth embodiment, “mesh ratio” with the embodiment can be pushed by 10K ¥ π +. _ J to improve the uniformity of M thickness. In FIG. 8 The size of the thinner areas of the four corners of the substrate is roughly the left and right sides of the substrate

相同。與基板中央區域之臈厚相比,75%以上之膜厚區 域’為基板面積之99·〇%之99〇〇 一,具有95%以上之膜厚 區域為基板面積之96.9%之9690 cm2。 (實施例5) 圖9A之概念的縱剖面圖係表示實施例5之成膜裝置,圖 9B之概念的平面圖係表示圖9A之成膜裝置内之排氣口配 置。如圖9A所#,在加熱器2之中央下方配置排氣管。 又,由圖9A與圖9B可以瞭解:沿著加熱器2下面之四邊配 置阻撞氣流之遮護板14。而’在沿著加熱器2四邊之4塊遮 護板14之各中央設有排氣口 51。由喷淋板1〇之孔向玻璃基 板1供應之反應氣體在被加熱之基板丨上形成透明導電膜, 其後,大致對稱地流向基板1之周邊,由4個排氣口 5丨被排 氣。又,在遮護板14與加熱器2之間之稜角及遮護板彼此 相接之稜角之部分也可具有微幅之間隙。 (實施例6) 圖10之概略的平面圖係作為實施例6,以圖9 a之成膜裝 置在1 mxl m之玻璃基板1形成氧化辞膜時之厚度分布。在 99619.doc -29- 200535275 此貫施例6中,在形成氧化鋅膜時,氣體壓力及氣體流量 與貫施例2之情形相同。圖1〇中之數值係以單位表示膜 厚之等高線。將圖10與圖6及圖8作比較時,可知:與實施 例2及4相比,在本實施例6中,可進一步改善膜厚均勻 性。在圖10中,基板四角之膜厚較薄區域之大小在基板之 左侧與右側大致相同。與基板中央區域之膜厚相比,75% 以上之膜厚區域,為基板面積之1〇〇%之1〇〇〇〇 cm2,具有 95%以上之膜厚區域為基板面積之99.4%之994〇 cm2。 (實施例7) 圖11A之概念的縱剖面圖係表示實施例7之成膜裝置,圖 11B之概念的平面圖係表示圖UA之成膜裝置内之排氣口 配置。此情形,成膜室3内之氣體由設於分歧排氣管15之 多數排氣口 52被吸入,通過分歧排氣管15及排氣管6被排 氣。此等多數排氣口 52係大致對稱配置於玻璃基板i之相 向之側邊附近,藉此,可在基板面中央大致對稱地施行氣 體之排氣。 在圖7及圖9A中,將排氣管6配置於加熱器2之中央下 方,但在本實施例7中,可將排氣管6配置於真空槽4之側 面。因此,將排氣管6配置於真空槽4之下有某些限制時, 採用本實施例7較為理想。又,在將多數基板平行地排在 水平方向而施行成膜之情形,為維持各基板面上之氣流之 均勻性,最好沿著基板之相向側面設置排氣口,排氣管6 也以如圖11A所示配置於真空槽4之側面為宜。 (實施例8) 99619.doc -30- 200535275 圖12之概略的平面圖係作為實施例8,以圖&quot;A之成膜裝 置在1 mxl m之玻璃基板丨形成氧化鋅膜時之厚度分布。在 此實施例8中,在形成氧化鋅膜時,氣體壓力及氣體流量 •與實施例2之情形相同。圖12中之數值係以帅單位表示膜 - 厚之等高線。將圖12與圖6、圖8、及圖1〇作比較時,與實 施例2、4及6相比,在本實施例8中,可進一步改善膜厚均 勻性。在圖12中,基板四角之臈厚較薄區域之大小在基板 之左側與右側大致相同。與基板中央區域之膜厚相比, • 75%以上之膜厚區域,為基板面積之100。/〇之10000 cm2, 具有95%以上之膜厚區域為基板面積之99 7%之997〇 cy。 (實施例9) 圖13A之概念的縱剖面圖係表示實施例9之成膜裝置,圖 13B之概念的平面圖係表示圖13A之成膜裝置中之排氣口 配置。如圖13A所示,在加熱器2之中央下方配置排氣管 6。又,由圖13A與圖13B可以瞭解:沿著加熱器2下面之 四邊配置阻擋氣流之遮護板14。而,在加熱器2之各角部 下設有排氣口 53。由噴淋板1〇之孔向玻璃基板丨供應之反 應氣體在被加熱之基板1上形成透明導電膜,其後,氣流 大致對稱地流向基板1之四角,由4個排氣口 53被排氣。 又,在遮護板14與加熱器2之間之稜角部分也可具有微幅 之間隙。 (實施例10) 圖14之概略的平面圖係作為實施例1〇,以圖13A之成膜 裝置在1 mxl m之玻璃基板丨形成氧化鋅膜時之厚度分布。 99619.doc 31 200535275 貝例1 0中’在形成氧化辞膜時,氣體壓力及氣體流 量,實之情形相同。圖14中之數值係以㈣單位表示 膜厚之等间線。將圖14與圖6、圖8、圖1〇及圖^作比較 時,可知:與實施例2、4、6及8相比,在本實施例1〇中, y進:步改善膜厚均勾性。在圖14中,基板四角之膜厚較 溥區域幾乎不存在。與基板中央區域之臈厚相比,75%以 上之膜厚區域,為基板面積之1〇〇%之i〇〇〇〇 cm2,具有 〇 乂上之膜厚區域為基板面積之100%之1 〇〇〇〇 cm2。 (實施例11) S之模式的σ彳面圖係表示實施例11之光電變換裝置。 此光電變換裝置係含有用圖5之成膜裝置形成於玻璃基板 16上之氧化鋅膜’以作為表面透明電極17。在該表面電極 π上,以電tCVD法形成含pin半導體接合之第一薄膜光 電變換單it 18及含pin半導體接合之第二薄膜光電變換單 元19再在其上,利用澉射法形成背面金屬電極2 〇。在此 光電變換裝置中,由玻璃基板16側入射之光被構成混合型 構造之第一光電變換單元丨8與第二光電變換單元丨9施行光 電變換。 第一光電變換單元18係由摻雜B之非晶質碳化矽之第 型半導體層18a、非晶質矽之第一真性半導體層丨8b、及摻 雜P之微晶矽之第一n型半導體層18c所構成。第二光電變 換單元19係由摻雜B之微晶矽之第二p型半導體層19a、多 晶石夕之第二真性半導體層19b、及摻雜p之微晶石夕之第二n 型半導體層19c所構成。與非晶質矽相比,多晶矽可吸收 99619.doc -32- 200535275 幸乂長波長之光’故未完全被第一真性半導體層1 8b吸收之 長波長之光可被第二真性半導體層19b吸收,而可改善光 電變換裝置之最大電力(pmax)。 此實施例11之光電變換裝置係利用91 cmX45.5 cm之面 積之玻璃基板形成,利用雷射將該基板上之半導體疊層構 造圖案化,而成為圖19所示之積體型光電變換模組之構 造。此時’電性串聯連接100段之光電變換胞11〇。此結 果,在本實施例1丨之大面積光電變換裝置之特性上,最大 電力(Pmax)為38·7 w,開放電壓(Voc)為131.9 V,短路電 流(Isc)為0.432 A,而曲線因子(FF)為0.679。 (比較例6) 作為比較例6,製作含利用圖3之成膜裝置形成之透明導 電膜作為表面電極之光電變換裝置。與實施例u相比,相 異之處在於在此比較例6之光電變換裝置中僅其透明導電 膜之形成方法。其結果,在比較例6之大面積光電變換裝 置之特性中,Pmax=3.6 w,v〇c=84 5 V,Isc=〇3〇4 A,而 FF=〇·140。即,比較例6之光電變換裝置之特性非常低; 相對地,可知實施例丨丨之光電變換裝置可大幅改善其特 性。 ’、、 (實施例12) 圖16之模式的剖面圖係表示實施例12之光電變換裝置。 本實施例12之光電變換裝置與圖15之實施例丨丨相異之處僅 在於在第二η型半導體層19c與背面電極2〇之間插入利用圖 3之成膜裝置形成之氧化鋅膜之背面反射層21。藉設置此 99619.doc »33- 200535275 背面反射層2 1,可使背面之光反射率增大。因此,未完全 被第一真性半導體層18b或第二真性半導體層19b吸收之長 波長之光可在第二η型半導體層19c與背面反射層21之界面 被反射而被利用於光電變換,故可提高光電變換裝置之特 性。又,在實施例12中,背面反射層21之厚度為80 nm。在 實施例12之大面積光電變換裝置之特性中,Pmax=41.5 W, Voc=132.5 V,Isc=〇.452 A,及 FF=0.693。其特性亦比實 施例11更高。 (實施例13) 圖17之模式的剖面圖係表示實施例13之光電變換裝置。 本實施例13之光電變換裝置與圖16之實施例12相異之處僅 在於在第一 η型半導體層i8c與第二p型半導體層i9a之間插 入利用圖5之成膜裝置形成之氧化鋅膜之中間層22。藉設 置此中間層22,可使未完全被第一真性半導體層1讣吸收 之光可在第一 η型半導體層i8c與中間層22之界面被反射而 在該第一真性半導體層1 8b中被利用於光電變換。又,透 過中間層22之光可被該中間層22之表面凹凸構造散射,故 可延長第一真性半導體層19b中之實質的光程長。因此, 在實施例13之光電變換裝置中,光之利用效率因中間層22 而提高,可更提高光電變換特性。又,在實施例13中,中 間層22之厚度為50 nm。在實施例13之大面積光電變換裝 置之特性中,Pmax=43.3 W,Voc=133.8 V,Isc=〇.463 A, 及FF=0.699。其特性亦比實施例12更高。 (實施例14) 99619.doc -34- 200535275 圖?之模式的剖面圖係表示實施例“之光電變換裝置。 之光電變換装置與圖15之實施例11相異之處僅 ^纟玻璃基板16與表面電極17間分散塗敷氧化矽η 1 立㈣成之底層23。透料電膜之表面電㈣之表面凹1 〜大T t可使光散射而延長光電變換裝置之實質的光程 ' 日大透明導電膜之厚度時,1亥透明導電臈之光吸 收扣耗也曰增加。因此,使用對光電變換裝置可利用之波 長之光大致透明之氧切微粒形成表面凹凸較大之底層 在底層23上利用圖5之成膜裝置形成透明導電膜之表 面電極17時’可_面抑制表面電極17之吸收損耗,一面增 大表面凹凸。底層23可利用將分散於凝膠狀之溶劑之心 石夕微粒塗敷在玻璃基體經锻燒所形成。此實施例Μ之大面 積光電、麦換裝置之特性為·· pmax=4l .9 w,3 v, Isc-0.461 A,及FF=0.687。其特性比實施例丨丨更高。 (實施例15) 在實施例15中,與實施例丨同樣利用圖5之成膜裝置形成 透明導電膜。但相異之處僅在於··實施例丨使用之圖以之 配管之距離A與B皆為0.15 m ,·對此,在實施例15中,距離 A與B均延長設定為1 m。 在實施例1中,即使成膜時間總共3〇〇小時,配管也不會 閉塞’但總共約達400小時之時,DEZ蒸氣之流量會變得 不穩定,粉體會附著於DEZ供應閥24而閉塞。另一方面, 在實施例15中,即使施行總共700小時以上之成膜,配管 也不會閉塞。其時,DEZ供應閥24與Ηβ供應閥25均未發 99619.doc -35- 200535275 生粉體引起之閉塞。 (實施例16) 在貝%例1 6中,也與實施例丨同樣利用圖5之成膜裝置形 成透月導電膜。但,在實施例i 6中,另外追加ι條與氣體 此口二間12合流之配管,並調製附加混合B2H6與η〗之反應 氣體。形成氧化鋅膜時,真空槽4内之壓力為1〇 pa、基板 溫度為150。。、DEZ蒸氣之流量為3〇〇 sccm、h2〇蒸氣之流 里為1000 seem、B2H62流量為i 5 sccm、H2之流量為5〇〇the same. Compared with the thickness of the central region of the substrate, more than 75% of the film thickness region 'is 99.0% of the substrate area, and more than 95% of the film thickness region is 96.9% of 9690 cm2 of the substrate area. (Embodiment 5) The longitudinal sectional view of the concept of Fig. 9A shows the film forming apparatus of Embodiment 5, and the plan view of the concept of Fig. 9B shows the exhaust port arrangement in the film forming apparatus of Fig. 9A. As shown in FIG. 9A, an exhaust pipe is arranged below the center of the heater 2. 9A and 9B, it can be understood that shielding plates 14 for blocking airflow are arranged along the four sides of the lower surface of the heater 2. An exhaust port 51 is provided at each center of the four shield plates 14 along the four sides of the heater 2. The reaction gas supplied to the glass substrate 1 from the hole of the shower plate 10 forms a transparent conductive film on the heated substrate 丨, and then flows approximately symmetrically to the periphery of the substrate 1 and is discharged through the four exhaust ports 5 丨. gas. Further, there may be a slight gap between the corners between the shield plate 14 and the heater 2 and the corners where the shield plates are in contact with each other. (Embodiment 6) The schematic plan view of Fig. 10 is taken as Embodiment 6, and the thickness distribution when the oxide film is formed on the glass substrate 1 of 1 mxl m with the film forming apparatus of Fig. 9a. In this sixth embodiment of 99619.doc -29-200535275, when the zinc oxide film is formed, the gas pressure and gas flow rate are the same as those in the second embodiment. The values in Fig. 10 are contour lines of the film thickness in units. Comparing Fig. 10 with Figs. 6 and 8, it can be seen that, compared with Examples 2 and 4, in this Example 6, the film thickness uniformity can be further improved. In FIG. 10, the sizes of the thinner film thickness areas at the four corners of the substrate are approximately the same on the left and right sides of the substrate. Compared with the film thickness of the central area of the substrate, a film thickness area of 75% or more is 1,000% of the substrate area and 1,000 cm2, and a film thickness area of 95% or more is 994% of the substrate area. cm2. (Embodiment 7) The longitudinal sectional view of the concept of Fig. 11A shows the film forming apparatus of Embodiment 7, and the plan view of the concept of Fig. 11B shows the exhaust port arrangement in the film forming apparatus of Fig. UA. In this case, the gas in the film forming chamber 3 is sucked in through the plurality of exhaust ports 52 provided in the branch exhaust pipe 15, and is exhausted through the branch exhaust pipe 15 and the exhaust pipe 6. Most of these exhaust ports 52 are arranged approximately symmetrically near the opposite sides of the glass substrate i, whereby the exhaust of the gas can be performed approximately symmetrically in the center of the substrate surface. 7 and 9A, the exhaust pipe 6 is arranged below the center of the heater 2. However, in the seventh embodiment, the exhaust pipe 6 may be arranged on the side of the vacuum tank 4. Therefore, when there are some restrictions on the arrangement of the exhaust pipe 6 under the vacuum tank 4, the seventh embodiment is preferred. In addition, in the case of forming a film by arranging a plurality of substrates in parallel in a horizontal direction, in order to maintain the uniformity of the air flow on each substrate surface, it is preferable to provide an exhaust port along the opposite side of the substrate, and the exhaust pipe 6 is also As shown in FIG. 11A, it is preferable to arrange on the side surface of the vacuum tank 4. (Embodiment 8) 99619.doc -30- 200535275 The schematic plan view of Fig. 12 is taken as embodiment 8, and the thickness distribution when a zinc oxide film was formed on a glass substrate of 1 mxl m with the film-forming device of "A" was formed. In the eighth embodiment, the gas pressure and the gas flow rate when forming the zinc oxide film are the same as those in the second embodiment. The values in Figure 12 represent the film-thickness contours in handsome units. When FIG. 12 is compared with FIG. 6, FIG. 8, and FIG. 10, the film thickness uniformity can be further improved in this example 8 as compared with the examples 2, 4, and 6. In FIG. 12, the sizes of the thinner and thicker areas at the four corners of the substrate are approximately the same on the left and right sides of the substrate. Compared with the film thickness in the center area of the substrate, 75% or more of the film thickness area is 100% of the substrate area. / 〇 of 10000 cm2, with a film thickness area of more than 95% is 99 7% of 997.0 cy of the substrate area. (Embodiment 9) The longitudinal sectional view of the concept of Fig. 13A shows the film-forming apparatus of Embodiment 9, and the plan view of the concept of Fig. 13B shows the exhaust port arrangement in the film-forming apparatus of Fig. 13A. As shown in FIG. 13A, an exhaust pipe 6 is arranged below the center of the heater 2. 13A and 13B, shield plates 14 for blocking airflow are arranged along four sides of the lower surface of the heater 2. As shown in FIG. Exhaust ports 53 are provided under the corners of the heater 2. The reaction gas supplied to the glass substrate from the hole of the shower plate 10 forms a transparent conductive film on the heated substrate 1, and thereafter, the air flows approximately symmetrically to the four corners of the substrate 1, and is exhausted by the four exhaust ports 53. gas. Further, the corner portion between the shield plate 14 and the heater 2 may have a slight gap. (Embodiment 10) The schematic plan view of Fig. 14 is taken as Embodiment 10, and the thickness distribution when a zinc oxide film was formed on a 1 mxl m glass substrate using the film forming apparatus of Fig. 13A. 99619.doc 31 200535275 In Example 10, when the oxide film was formed, the gas pressure and gas flow were the same. The numerical values in Fig. 14 are the isometric lines of the film thickness in units of ㈣. Comparing FIG. 14 with FIG. 6, FIG. 8, FIG. 10, and FIG. ^, It can be seen that compared with Examples 2, 4, 6, and 8, in this Example 10, y is further improved: film thickness is further improved Uniformity. In Fig. 14, the film thickness at the four corners of the substrate is almost non-existent. Compared with the thickness of the central area of the substrate, more than 75% of the film thickness area is 1000% of the substrate area, and 100% of the substrate area is 100% of the substrate area. 〇〇〇cm2. (Embodiment 11) The σ 彳 plane view of the S mode shows the photoelectric conversion device of Embodiment 11. This photoelectric conversion device includes, as a surface transparent electrode 17, a zinc oxide film 'formed on a glass substrate 16 using the film forming device of Fig. 5. On the surface electrode π, a first thin-film photoelectric conversion unit 18 including a pin semiconductor junction and a second thin-film photoelectric conversion unit 19 including a pin semiconductor junction are formed by an electric tCVD method, and a back metal is formed thereon by an epitaxial method. Electrode 2 〇. In this photoelectric conversion device, light incident from the glass substrate 16 side is subjected to photoelectric conversion by the first photoelectric conversion unit 8 and the second photoelectric conversion unit 9 having a hybrid structure. The first photoelectric conversion unit 18 is composed of a first type semiconductor layer 18a of amorphous silicon carbide doped with B, a first true semiconductor layer of amorphous silicon 丨 8b, and a first n type of microcrystalline silicon doped with P. The semiconductor layer 18c is configured. The second photoelectric conversion unit 19 is composed of a second p-type semiconductor layer 19a doped with microcrystalline silicon doped with B, a second true semiconductor layer 19b with polycrystalline silicon, and a second n-type doped with microcrystalline silicon. The semiconductor layer 19c is configured. Compared with amorphous silicon, polycrystalline silicon can absorb 99619.doc -32- 200535275. Fortunately, long-wavelength light is not completely absorbed by the first true semiconductor layer 18b, so it can be absorbed by the second true semiconductor layer 19b. Absorption, which can improve the maximum power (pmax) of the photoelectric conversion device. The photoelectric conversion device of this embodiment 11 is formed using a glass substrate having an area of 91 cm × 45.5 cm, and a semiconductor stacked structure on the substrate is patterned by laser to form a integrated photoelectric conversion module as shown in FIG. 19 Of the structure. At this time, 100 segments of the photoelectric conversion cells 11 are electrically connected in series. As a result, in the characteristics of the large-area photoelectric conversion device of Example 1 丨, the maximum power (Pmax) was 38.7 w, the open voltage (Voc) was 131.9 V, the short-circuit current (Isc) was 0.432 A, and the curve The factor (FF) is 0.679. (Comparative Example 6) As Comparative Example 6, a photoelectric conversion device including a transparent conductive film formed using the film forming apparatus of Fig. 3 as a surface electrode was produced. Compared with Example u, the difference lies in the method of forming only the transparent conductive film in the photoelectric conversion device of Comparative Example 6. As a result, among the characteristics of the large-area photoelectric conversion device of Comparative Example 6, Pmax = 3.6 w, voc = 84 5 V, Isc = 〇3〇4 A, and FF = 0.40. That is, the characteristics of the photoelectric conversion device of Comparative Example 6 are very low; relatively, it can be seen that the photoelectric conversion device of Example 丨 can significantly improve its characteristics. ', (Embodiment 12) A cross-sectional view in the mode of Fig. 16 shows a photoelectric conversion device according to Embodiment 12. The photoelectric conversion device of the twelfth embodiment differs from the embodiment of FIG. 15 only in that a zinc oxide film formed by the film-forming device of FIG. 3 is inserted between the second n-type semiconductor layer 19c and the back electrode 20. The rear surface reflection layer 21. By setting this 99619.doc »33- 200535275 back reflective layer 21, the light reflectance of the back can be increased. Therefore, long-wavelength light that is not completely absorbed by the first true semiconductor layer 18b or the second true semiconductor layer 19b can be reflected at the interface between the second n-type semiconductor layer 19c and the back reflective layer 21 and used for photoelectric conversion. Can improve the characteristics of the photoelectric conversion device. Moreover, in Example 12, the thickness of the back reflection layer 21 was 80 nm. In the characteristics of the large-area photoelectric conversion device of Example 12, Pmax = 41.5 W, Voc = 132.5 V, Isc = 0.452 A, and FF = 0.693. Its characteristics are also higher than those of Example 11. (Embodiment 13) A cross-sectional view in the mode of FIG. 17 shows a photoelectric conversion device according to Embodiment 13. The photoelectric conversion device of the thirteenth embodiment is different from the twelfth embodiment of FIG. 16 only in that the oxidation formed by the film forming device of FIG. 5 is inserted between the first n-type semiconductor layer i8c and the second p-type semiconductor layer i9a Middle layer 22 of zinc film. By providing this intermediate layer 22, light that is not completely absorbed by the first true semiconductor layer 1 讣 can be reflected at the interface between the first n-type semiconductor layer i8c and the intermediate layer 22 and be reflected in the first true semiconductor layer 18b. Used for photoelectric conversion. In addition, since the light passing through the intermediate layer 22 can be scattered by the uneven structure on the surface of the intermediate layer 22, the substantial optical path length in the first true semiconductor layer 19b can be extended. Therefore, in the photoelectric conversion device of Example 13, the utilization efficiency of light is improved by the intermediate layer 22, and the photoelectric conversion characteristics can be further improved. In Embodiment 13, the thickness of the intermediate layer 22 is 50 nm. In the characteristics of the large-area photoelectric conversion device of Example 13, Pmax = 43.3 W, Voc = 133.8 V, Isc = 0.463 A, and FF = 0.699. Its characteristics are also higher than those of Example 12. (Example 14) 99619.doc -34- 200535275 Figure? The cross-sectional view of the mode shows the photoelectric conversion device of the embodiment ". The difference between the photoelectric conversion device and the embodiment 11 of Fig. 15 is that the silicon oxide η 1 is dispersedly applied between the glass substrate 16 and the surface electrode 17.成 的 底 底 23. The surface of the transmissive electrical film is concave on the surface of the electrode 1 ~ T T can scatter light and extend the substantial optical path of the photoelectric conversion device. When the thickness of the transparent conductive film is large, it is transparent and conductive. The light absorption deduction is also increased. Therefore, a bottom layer with a large surface unevenness is formed using oxygen-cut particles that are substantially transparent to light of a wavelength available to the photoelectric conversion device. On the bottom layer 23, a transparent conductive film is formed using the film-forming device of FIG. When the surface electrode 17 is used, the surface can suppress the absorption loss of the surface electrode 17 and increase the surface unevenness. The bottom layer 23 can be formed by coating the glass substrate with calcareous particles dispersed in a gel-like solvent on the glass substrate. The characteristics of the large-area photovoltaic and wheat-changing device of this embodiment M are: pmax = 41.9 w, 3 v, Isc-0.461 A, and FF = 0.687. Its characteristics are higher than those of the embodiment. (Implementation Example 15) In Example 15, and Example丨 The transparent conductive film is also formed using the film-forming device of FIG. 5. However, the difference lies only in the embodiment. The piping distances A and B used are both 0.15 m. In this regard, in Example 15 The distance A and B are both extended to 1 m. In Example 1, even if the film formation time is 300 hours in total, the piping will not be blocked. However, when the total time is about 400 hours, the flow rate of the DEZ vapor will change. If it is unstable, the powder adheres to the DEZ supply valve 24 and is blocked. On the other hand, in Example 15, even if the film formation is performed for a total of 700 hours or more, the piping will not be blocked. At this time, the DEZ supply valve 24 and Ηβ None of the supply valves 25 was 99619.doc -35- 200535275 occlusion caused by raw powder. (Example 16) In Example 16 as well, in the same manner as in Example 丨, the film-forming device of FIG. 5 was used to form translucent conductivity. However, in Example i 6, an additional twelve piping which is combined with the gas and two ports 12 was added, and an additional mixed reaction gas of B2H6 and η was prepared. When the zinc oxide film was formed, the pressure in the vacuum tank 4 10 Pa, substrate temperature 150 ..., DEZ vapor flow rate is 300 sccm h2〇 vapor inside his ilk to 1000 seem, B2H62 flow i 5 sccm, flow rate of H2 is 5〇〇

seem、Ar之流量為DEZ供應管7與H2〇供應管8合計5〇〇 seem。在實施例16中,藉供應比札,可降低透明導電膜之 薄膜電阻。又,藉供應H2,在低成膜壓力下仍可維持良好 之基板溫度之均勻性,不但透明導電膜之厚度均勻性,且 透光率及薄膜電阻之均勻性皆可提高。 (實施例17) 圖26A之概念的縱剖面圖係表示實施例17之成膜裝置, 圖26B之概念的縱剖面圖係表示圖26A之成膜裝置中之排 氣口配置。此實施例17之成膜裝置類似於圖13 A與圖13β 所示之實施例9之成膜裴置,但實施例9之成膜裝置係水平 型,相對地,實施例17之成膜裝置則為縱型。 又,圖26A之成膜裝置具有平行之2塊喷淋板1〇,故在面 對該等2塊噴淋板10配置多數基板丨時,可有效率地成膜。 為使反應氣體由兩側之噴淋板10均勻地噴出,使反應氣配 管11延伸至喷淋板10之中央附近,由該處將反應氣體供應 至噴淋板。喷淋板10之表面受到溫度控制,故延伸至喷淋 99619.doc -36- 200535275 板内侧之反應氣配管丨丨之部分在該處即使附設壁面加熱器 13,也可維持與反應氣配管丨丨大致相同之溫度。 在縱型之成膜裝置中,基板丨之主面配置於垂直方向, 故即使產生附著於成膜室之内壁、喷淋板丨〇、加熱器2等 之沉積物剝離之粉塵,粉塵也不會掉落附著於基板主面 上,故可抑制形成於基板丨上之透明導電膜發生如針孔般 之夹fe因此,與水平型之成膜裝置相比,縱型成膜裝置 可長柃間不必轭行成膜室内之清掃,可穩定地繼續成膜。The flow rates of seem and Ar are the total of 500 seem for the DEZ supply pipe 7 and the H20 supply pipe 8. In the sixteenth embodiment, the sheet resistance of the transparent conductive film can be reduced by the supply of the bazaar. In addition, by supplying H2, the uniformity of the substrate temperature can be maintained under a low film forming pressure, not only the thickness uniformity of the transparent conductive film, but also the uniformity of light transmittance and sheet resistance. (Embodiment 17) The longitudinal sectional view of the concept of Fig. 26A shows the film-forming apparatus of Embodiment 17, and the longitudinal sectional view of the concept of Fig. 26B shows the arrangement of exhaust ports in the film-forming apparatus of Fig. 26A. The film-forming device of this embodiment 17 is similar to the film-forming device of embodiment 9 shown in FIGS. 13A and 13β, but the film-forming device of embodiment 9 is a horizontal type. In contrast, the film-forming device of embodiment 17 It is vertical. In addition, the film forming apparatus of FIG. 26A has two shower plates 10 in parallel. Therefore, when a plurality of substrates are arranged facing the two shower plates 10, the film can be efficiently formed. In order to spray the reaction gas uniformly from the shower plates 10 on both sides, the reaction gas pipe 11 is extended to the vicinity of the center of the shower plate 10, and the reaction gas is supplied to the shower plate from there. The surface of the shower plate 10 is controlled by temperature, so it extends to the reaction gas piping inside the shower 99619.doc -36- 200535275. Even if a wall heater 13 is attached, the reaction gas piping can be maintained there.丨 roughly the same temperature. In the vertical film-forming device, the main surface of the substrate 丨 is arranged in the vertical direction, so even if dust is peeled off from the deposits attached to the inner wall of the film-forming chamber, the shower plate 丨 0, and the heater 2, the dust is not It will fall and adhere to the main surface of the substrate, so that pinhole-like pinholes can be prevented from occurring on the transparent conductive film formed on the substrate. Therefore, the vertical film-forming device can be longer than the horizontal film-forming device. There is no need to yoke the cleaning in the film forming chamber, and the film formation can be continued stably.

又,在本實施例17之成膜裝置中,可面對丨塊噴淋板⑺ 配置2塊0·5 mxl m面積之基板(參照圖26B),該情形,可同 時在4塊基板i上成膜。又,利用本實施㈣之成膜裝置形 成之透明導電膜具有與實施例9同樣均勻之膜厚分布。 (實施例18) 圖27A之概念的縱剖面圖係表示實施例18之成膜裝置, 圖27B之概念的縱剖面圖係表示圖27八之成膜裝置中之排 氣口配置。此實施例18之縱型成膜裝置與圖&quot;A、圖 11B、及圖26A相t匕時,可以獲悉含有實施例7之一部分之 特徵與實施例之-部分之特徵。依據此實施_之成膜 裝置’可面對4塊噴淋板1〇配置例士。_饥面積之 塊’可同時在4塊大面積基板工上成膜。又,本實施韻之 成膜裝置形成之透明導電膜具有與實施例7同樣均勻之膜 厚分布。 ' 在使用有機金屬蒸氣與氧化劑 【產業上之可利用性】 如上所述,依據本發明 99619.doc -37- 200535275 蒸氣之低壓熱CVD中,可形成大面 勝甘 、:勻之透明導電 膜。—果,可提供含透明導電膜之大面積之、 提供改善特性之大面積之光電變換裝置。 己” 【圖式簡單說明】 圖1係表示形成透明導電膜之用之以往之成 例之概念圖。 、 圖2係圖1之成膜裝置所形成之透明導電膜之厚度分 圖0In addition, in the film-forming apparatus of this embodiment 17, two spraying plates 面对 can be arranged to face two substrates with an area of 0.5 mxl m (see FIG. 26B). In this case, four substrates i can be simultaneously installed. Film formation. The transparent conductive film formed by the film forming apparatus of this embodiment has a uniform film thickness distribution similar to that of Example 9. (Embodiment 18) The longitudinal sectional view of the concept of Fig. 27A shows the film-forming apparatus of Embodiment 18, and the longitudinal sectional view of the concept of Fig. 27B shows the exhaust port arrangement in the film-forming apparatus of Fig. 27A. When the vertical film-forming apparatus of this embodiment 18 is in accordance with the drawings "A, 11B, and 26A, it can be understood that the features including one part of the embodiment 7 and the features of the -part of the embodiment are included. According to this implementation, the film-forming device 'can face 4 spraying plates 10 and be configured. _ Block of hungry area 'can be formed on 4 large-area substrates at the same time. The transparent conductive film formed by the film forming apparatus of this embodiment has a uniform film thickness distribution as in Example 7. '' In the use of organometallic vapor and oxidant [Industrial availability] As described above, according to the present invention, the low-pressure thermal CVD of 99619.doc -37- 200535275 vapor can form a large transparent conductive film . —As a result, it is possible to provide a large-area photoelectric conversion device containing a transparent conductive film and a large area with improved characteristics. [Simple illustration] Figure 1 is a conceptual diagram showing a conventional example of forming a transparent conductive film. Figure 2 is a thickness analysis of the transparent conductive film formed by the film forming apparatus of Figure 1 Figure 0

圖3係表示形成透料電膜之用之以往之成膜裝置之另 一例之概念圖。 圖4係圖3之成膜裝置所形成之透明導電膜之厚度八 圖。 圖5係本發明之一實施例之成膜裝置之概念圖。 圖ό係圖5之成膜裝置所形成之透明導電膜之厚度分 圖。 圖7係本發明之另一實施例之成膜裝置之概念圖。 圖8係圖7之成膜裝置所形成之透明導電膜之厚度分布 圖0 圖9Α係本發明之又另一實施例之成膜裝置之概念的縱剖 面圖。 圖9Β係表不圖9Α之成膜裝置中之排氣口配置之概念的 平面圖。 圖10係圖9 A之成膜裝置所形成之透明導電膜之厚度分布 圖0 99619.doc -38- 200535275 圖11A係本發明之又另一實施例之成膜裝置之概念的縱 剖面圖。 圖11B係表示圖nA之成膜裝置中之排氣口配置之概念 的平面圖。 圖12係圖11A之成膜裝置所形成之透明導電膜之厚度分 布圖。 圖13A係本發明之又另—實施例之成膜裝置之概念的縱 剖面圖。 圖13B係表示圖13A之成膜裝置中之排氣口配置之概念 的平面圖。 圖14係圖13A之成膜裝置所形成之透明導電膜之厚度分 布圖。 圖15係表示本發明之又另一實施例之光電變換裝置之模 式的剖面圖。 圖16係表示本發明之又另一實施例之光電變換裝置之模 式的剖面圖。 圖17係表示本發明之又另一實施例之光電變換裝置之模 式的剖面圖。 圖18係表示本發明之又另一實施例之光電變換裝置之模 式的剖面圖。 圖19係表示本發明之又另一實施例之大面積光電變換裝 置之模式的剖面圖。 圖20係表示以往之成膜裝置之另一例之概念圖。 圖21係表示本發明之成膜裝置之氣體混合空間附近之配 99619.doc -39- 200535275 管之模式圖。 圖22係表示DEZ供應管中依存於與氣體混合空間之距離 而存在之H20之相對密度之曲線圖。 圖23係蒸發氣化器之概念圖。 圖24係起泡氣化器之概念圖。 圖25(a)-(b)係喷霧氣化器之概念圖。 圖26A係本發明之又另一實施例之成膜裝置之概念的縱 剖面圖。 p 圖26B係表示圖26A之成膜裝置中之排氣口配置之概念 的縱剖圖。 圖27A係本發明之又另一實施例之成膜裝置之概念的縱 剖面圖。 圖27B係表示圖27A之成膜裝置中之排氣口配置之概念 的縱剖圖。 又,在本案之圖式中,同一參照符號係表示同一部分或 相當部分。 • 【主要元件符號說明】 1 玻璃基板 2 加熱器 3 成膜室 4 真空槽 5 、 51 、 52 、 53 排氣口 6 排氣管 7 DEZ供應管 99619.doc -40- 200535275 8 H20供應管 9 擴散箱 10 喷淋板 11 反應氣配管 12 氣體混合空間 13 壁面加熱器 14 遮護板 15 分歧排氣管 16 玻璃基板 17 表面電極 18 第一光電變換單元 18a 第一 P型半導體層 18b 第一真性半導體層 18c 第一 η型半導體層 19 第二光電變換單元 19a 第二ρ型半導體層 19b 第二真性半導體層 19c 第二η型半導體層 20 背面電極 21 背面反射層 22 中間層 23 底層 24 DEZ供應閥 25 Η20供應閥 99619.doc -41 - 200535275Fig. 3 is a conceptual diagram showing another example of a conventional film-forming apparatus for forming a transparent electric film. FIG. 4 is an eight diagram of the thickness of the transparent conductive film formed by the film forming apparatus of FIG. 3. FIG. FIG. 5 is a conceptual diagram of a film forming apparatus according to an embodiment of the present invention. FIG. 6 is a thickness map of the transparent conductive film formed by the film forming apparatus of FIG. 5. FIG. 7 is a conceptual diagram of a film forming apparatus according to another embodiment of the present invention. Fig. 8 is a thickness distribution of a transparent conductive film formed by the film forming apparatus of Fig. 7; Fig. 9A is a longitudinal sectional view showing the concept of a film forming apparatus according to another embodiment of the present invention. Fig. 9B is a plan view showing the concept of the arrangement of exhaust ports in the film forming apparatus of Fig. 9A. Fig. 10 is a thickness distribution of a transparent conductive film formed by the film forming apparatus of Fig. 9A. Fig. 0 99619.doc -38- 200535275 Fig. 11A is a longitudinal sectional view showing the concept of a film forming apparatus according to another embodiment of the present invention. Fig. 11B is a plan view showing the concept of the arrangement of exhaust ports in the film forming apparatus of Fig. NA. Fig. 12 is a thickness distribution diagram of a transparent conductive film formed by the film forming apparatus of Fig. 11A. Fig. 13A is a longitudinal sectional view showing the concept of a film forming apparatus according to still another embodiment of the present invention. Fig. 13B is a plan view showing the concept of the arrangement of exhaust ports in the film forming apparatus of Fig. 13A. Fig. 14 is a thickness distribution diagram of a transparent conductive film formed by the film forming apparatus of Fig. 13A. Fig. 15 is a sectional view showing a mode of a photoelectric conversion device according to still another embodiment of the present invention. Fig. 16 is a sectional view showing a mode of a photoelectric conversion device according to still another embodiment of the present invention. Fig. 17 is a sectional view showing a mode of a photoelectric conversion device according to still another embodiment of the present invention. Fig. 18 is a sectional view showing a mode of a photoelectric conversion device according to still another embodiment of the present invention. Fig. 19 is a sectional view showing a mode of a large-area photoelectric conversion device according to still another embodiment of the present invention. FIG. 20 is a conceptual diagram showing another example of a conventional film forming apparatus. Fig. 21 is a schematic diagram showing the distribution of 99619.doc -39- 200535275 tubes near the gas mixing space of the film forming apparatus of the present invention. Fig. 22 is a graph showing the relative density of H20 existing in the DEZ supply pipe depending on the distance from the gas mixing space. Figure 23 is a conceptual diagram of an evaporative gasifier. Figure 24 is a conceptual diagram of a bubble gasifier. Figures 25 (a)-(b) are conceptual diagrams of a spray gasifier. Fig. 26A is a longitudinal sectional view showing the concept of a film forming apparatus according to still another embodiment of the present invention. p Fig. 26B is a longitudinal sectional view showing the concept of the arrangement of exhaust ports in the film forming apparatus of Fig. 26A. Fig. 27A is a longitudinal sectional view showing the concept of a film forming apparatus according to still another embodiment of the present invention. Fig. 27B is a longitudinal sectional view showing the concept of the arrangement of exhaust ports in the film forming apparatus of Fig. 27A. In the drawings of the present case, the same reference signs denote the same or corresponding parts. • [Description of main component symbols] 1 Glass substrate 2 Heater 3 Film forming chamber 4 Vacuum tanks 5, 51, 52, 53 Exhaust port 6 Exhaust pipe 7 DEZ supply pipe 99619.doc -40- 200535275 8 H20 supply pipe 9 Diffusion box 10 Shower plate 11 Reactive gas piping 12 Gas mixing space 13 Wall heater 14 Sheath plate 15 Branch exhaust pipe 16 Glass substrate 17 Surface electrode 18 First photoelectric conversion unit 18a First P-type semiconductor layer 18b First authenticity Semiconductor layer 18c First n-type semiconductor layer 19 Second photoelectric conversion unit 19a Second p-type semiconductor layer 19b Second true semiconductor layer 19c Second n-type semiconductor layer 20 Back electrode 21 Back reflective layer 22 Intermediate layer 23 Bottom layer 24 DEZ supply Valve 25 Η 20 Supply valve 99619.doc -41-200535275

26 加熱器 27 槽 28 液體材料 29 蒸氣 30 氣體質量流控制器 31 重量計 32 恆溫槽 33 氣泡 34 氣體質量流控制器 35 液體質量流控制器 36 混合器 37 Ar供應管 38 液體材料供應管 39 微小孔 40 霧狀液體材料 41 氣化氣體供應管 71 加熱器 81 加熱器 101 積體型薄膜光電變換模組 102 玻璃基板 103 表面電極層 104a 第一光電變換單元 104b 第二光電變換單元 106 背面電極層 99619.doc -42- 200535275 110 光電變換胞 121 第一分離溝 122 第二分離溝 123 連接溝 99619.doc26 Heater 27 Tank 28 Liquid material 29 Vapor 30 Gas mass flow controller 31 Gravimeter 32 Thermostatic bath 33 Bubble 34 Gas mass flow controller 35 Liquid mass flow controller 36 Mixer 37 Ar supply pipe 38 Liquid material supply pipe 39 Micro Hole 40 Mist liquid material 41 Vaporized gas supply tube 71 Heater 81 Heater 101 Integrated thin-film photoelectric conversion module 102 Glass substrate 103 Surface electrode layer 104a First photoelectric conversion unit 104b Second photoelectric conversion unit 106 Back electrode layer 99619 .doc -42- 200535275 110 photoelectric conversion cell 121 first separation groove 122 second separation groove 123 connection groove 99619.doc

Claims (1)

200535275 申請專利範圍: 1. 種成膜裝置’其特徵在於包含: 利用CVD將透明導電膜沉積於具有22〇 cm2以上之面積 之底層上用之成膜室; 輸送含有機金屬蒸氣之第丨氣體之第丨氣體管; 輸送含氧化劑蒸氣之第2氣體之第2氣體管; 結合前述第1與前述第2氣體管以混合前述第丨與前述 弟2氣體用之氣體混合空間; ; 將在前述氣體混合空間被混合之反應氣體導入前 膜室内之氣體導入手段;及 由則述成膜室排出排氣用之排氣裝置者。 2·如明求項1之成膜裝置,其中前述氣體導入手段係含 數氣體放出子丨夕+、从α ,、 r 淋板’可將前述反應氣體控制於 2〇〜i〇〇c之範圍内之溫度者。 3. 如清求項1之成腔姑 -. 以上之剖面積者,/、“述氣體混合空間係具有 99619.doc 200535275 保持手段或加熱器者。 δ·:請求们之成膜裝置’其中含有保持前述底層用之底 :保持手段或保持前述底層用之加熱器,前述排氣裝置 係連接於面對前述底層保持手段或前述加熱m設 . 置之排氣口者。 9·如請求項2之成㈣置,其中關於前述喷淋板之中心, 對稱地將多數排氣口設於前述成膜室内者。 1〇·種成膜方法,其4寺徵在於:其係利用CVD將透明導電 • 膜沉積於配置於成臈室内之底層上者;且 在含有機金屬蒸氣之第丨氣體與含氧化劑蒸氣之第2氣 體被導人前述成膜室内之前,在氣體混合空間被混合成 反應氣體者。 11. 如請求項10之成膜方法,其中前述透明導電膜係氧化辞 者。 12. 如請求項H)之成膜方法’其中前述有機金屬蒸氣係含烧 基辞者。 • 13.如請求項1〇之成膜方法’其中前述氧化劑蒸氣係含有選 擇自水、氧、二氧化碳、一氧化碳、氧化二氮、二氧化 氮、二氧化硫、五氧化二氮、醇類(R(〇H))、酮類 (R(CO)R’)、醚類(R0R,)、醛類(R(c〇H))、醯胺類 ((RCO)x(NH3-x)、χ=:ι,2,3)及亞石風類(R(s〇)R,)(其中,r 及RW系烧基。)中至少一種者。 14.如請求項10之成膜方法,其中輸送至前述氣體混合空間 之前述有機金屬蒸氣與前述氧化劑蒸氣之至少一方係與 99619.doc 200535275 載氣混合者。 15.如請求項14之成 甘七义、々士 M ^ 风暝方法,其中則述有機金屬蒸氣與前述 氧化劑瘵氣之至少-方係被起泡法所氣化者。 #月长^14之成膜方法,其中前述有機金屬蒸氣與前述 乳化劑祭氣之至少—方係被喷霧氣化器所氣化者。 17.如請求項1()之成臈方法,纟中由前述氣體混合空間至前 述成臈至内之氣流路徑係被控制於20〜l〇(TC之範圍内之 溫度者。 18. 如請求項1〇之成膜方法,其中前述反應氣體係經由含多 數氣體放出孔之噴淋板而被導入前述成膜室内者。 19. 如請求項18之成膜方法,其中前述噴淋板係可將前述反 應氣體控制於20〜10(rc之範圍内之溫度者。 2 0 ·如6奢求項1 〇之成膜方、、木 甘 a 乂 膜方法其中别述氣體混合空間内之壓 力係被调整於1 3 〇 〇 p a以下者。 21. -種光電變換裝置’其特徵在於:在表面電極中 用請求項10之成膜方法所形成之透明導電膜者。 22· -種光電變«置,其特徵在於:在背面電極 用請求項10之成膜方法所形成之透明導電膜者。 23. -種光電變換裝置’其特徵在於:含有利用請求項w 成膜方法所形成之透明導電膜作、之 者。 ^卞守蔽臂甲之中間層 99619.doc200535275 The scope of the patent application: 1. A film-forming device, which is characterized by: a film-forming chamber for depositing a transparent conductive film on a bottom layer having an area of more than 22 cm2 by CVD; and conveying a gas containing organic metal vapor The first gas pipe; the second gas pipe that conveys the second gas containing oxidant vapor; the first and second gas pipes are combined to mix the gas mixing space for the first and second gas; A gas introduction means for introducing the mixed reaction gas into the front membrane chamber in the gas mixing space; and an exhaust device for exhausting the exhaust gas from the film forming chamber. 2. The film-forming device as described in item 1 above, wherein the gas introduction means is composed of a number of gas emission elements, such as +, from α, and r, which can control the above-mentioned reaction gas to between 20 and 100. Temperature within the range. 3. For example, if the above-mentioned cross-sectional area of item 1 is required, "The gas mixing space has a 99619.doc 200535275 holding means or a heater. Δ ·: The film-forming device of the requester 'which Contains a base for holding the aforementioned bottom layer: a holding means or a heater for holding the aforementioned bottom layer, the exhaust device is connected to an exhaust port facing the aforementioned base holding means or the aforementioned heating device. 9 · If requested The setting of 2 is a method in which the center of the aforementioned shower plate is provided with a plurality of exhaust ports symmetrically in the aforementioned film forming chamber. 10. A film forming method, the fourth characteristic of which is that it uses CVD to make transparent Conductive • The film is deposited on the bottom layer arranged in the forming chamber; and before the second gas containing organic metal vapor and the second gas containing oxidant vapor are introduced into the aforementioned film forming chamber, they are mixed into a reaction in the gas mixing space. Gases. 11. The film-forming method according to claim 10, wherein the aforementioned transparent conductive film is oxidized. 12. The film-forming method according to claim H), wherein the aforementioned organometallic vapors are based on sintered radicals. • 13 .Such as Method for film formation of term 10, wherein said oxidant vapor system contains selected from water, oxygen, carbon dioxide, carbon monoxide, dinitrogen oxide, nitrogen dioxide, sulfur dioxide, dinitrogen pentoxide, alcohols (R (〇H)), Ketones (R (CO) R '), ethers (ROR,), aldehydes (R (co)), amidoamines ((RCO) x (NH3-x), χ =: ι, 2, 3) and at least one of the sub-stone breeze (R (s〇) R,) (wherein r and RW are calcined groups.) 14. The film-forming method according to claim 10, wherein the film is conveyed to the aforementioned gas mixing space. At least one of the aforementioned organometallic vapor and the aforementioned oxidant vapor is a mixture with a carrier gas of 99619.doc 200535275. 15. The method of Gan Qiyi and Zhishi M ^ Fengyao as claimed in claim 14, wherein the organometallic vapor and the aforementioned oxidant At least-the side of radon gas is gasified by the foaming method. # 月 长 ^ 14The film formation method, where at least-the aforementioned organometal vapor and the emulsifier sacrificial gas are gasified by the spray gasifier 17. In accordance with the method of claim 1 (), the airflow path from the aforementioned gas mixing space to the aforementioned agent to within Those controlled at a temperature in the range of 20 to 10 ° C. 18. The film forming method as claimed in item 10, wherein the aforementioned reaction gas system is introduced into the aforementioned film forming chamber through a shower plate containing most gas release holes. 19. If the film-forming method of item 18 is requested, wherein the aforementioned shower plate can control the aforementioned reaction gas to a temperature in the range of 20 to 10 (rc). 2 0 · Such as 6 extravagant film-forming of 1 〇 Fang, Mugan a 乂 membrane method, in which the pressure in the gas mixing space is adjusted to less than 13,000pa. 21. A photoelectric conversion device ', characterized in that a transparent conductive film is formed on a surface electrode by the film-forming method of claim 10. 22 ·-A type of photoelectric transformer, characterized in that it is a transparent conductive film formed on the back electrode by the film-forming method of claim 10. 23. A photoelectric conversion device ', characterized in that it comprises a transparent conductive film formed by a film forming method according to claim w. ^ 卞 Guarding the middle layer of the armguards 99619.doc
TW094104914A 2004-02-20 2005-02-18 Method and apparatus for forming transparent conductive film TW200535275A (en)

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