[go: up one dir, main page]

TW201216491A - Method for thin film silicon photovoltaic cell production - Google Patents

Method for thin film silicon photovoltaic cell production Download PDF

Info

Publication number
TW201216491A
TW201216491A TW100131603A TW100131603A TW201216491A TW 201216491 A TW201216491 A TW 201216491A TW 100131603 A TW100131603 A TW 100131603A TW 100131603 A TW100131603 A TW 100131603A TW 201216491 A TW201216491 A TW 201216491A
Authority
TW
Taiwan
Prior art keywords
layer
deposition
battery
flow rate
type layer
Prior art date
Application number
TW100131603A
Other languages
Chinese (zh)
Inventor
Hanno Goldbach
Tobias Roschek
Roman Kravets
Original Assignee
Oerlikon Solar Ag
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Oerlikon Solar Ag filed Critical Oerlikon Solar Ag
Publication of TW201216491A publication Critical patent/TW201216491A/en

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F77/00Constructional details of devices covered by this subclass
    • H10F77/70Surface textures, e.g. pyramid structures
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F10/00Individual photovoltaic cells, e.g. solar cells
    • H10F10/10Individual photovoltaic cells, e.g. solar cells having potential barriers
    • H10F10/17Photovoltaic cells having only PIN junction potential barriers
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F10/00Individual photovoltaic cells, e.g. solar cells
    • H10F10/10Individual photovoltaic cells, e.g. solar cells having potential barriers
    • H10F10/17Photovoltaic cells having only PIN junction potential barriers
    • H10F10/172Photovoltaic cells having only PIN junction potential barriers comprising multiple PIN junctions, e.g. tandem cells
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F71/00Manufacture or treatment of devices covered by this subclass
    • H10F71/10Manufacture or treatment of devices covered by this subclass the devices comprising amorphous semiconductor material
    • H10F71/103Manufacture or treatment of devices covered by this subclass the devices comprising amorphous semiconductor material including only Group IV materials
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F71/00Manufacture or treatment of devices covered by this subclass
    • H10F71/121The active layers comprising only Group IV materials
    • H10F71/1224The active layers comprising only Group IV materials comprising microcrystalline silicon
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F77/00Constructional details of devices covered by this subclass
    • H10F77/10Semiconductor bodies
    • H10F77/16Material structures, e.g. crystalline structures, film structures or crystal plane orientations
    • H10F77/162Non-monocrystalline materials, e.g. semiconductor particles embedded in insulating materials
    • H10F77/164Polycrystalline semiconductors
    • H10F77/1642Polycrystalline semiconductors including only Group IV materials
    • H10F77/1645Polycrystalline semiconductors including only Group IV materials including microcrystalline silicon
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F77/00Constructional details of devices covered by this subclass
    • H10F77/20Electrodes
    • H10F77/244Electrodes made of transparent conductive layers, e.g. transparent conductive oxide [TCO] layers
    • H10F77/251Electrodes made of transparent conductive layers, e.g. transparent conductive oxide [TCO] layers comprising zinc oxide [ZnO]
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F77/00Constructional details of devices covered by this subclass
    • H10F77/40Optical elements or arrangements
    • H10F77/42Optical elements or arrangements directly associated or integrated with photovoltaic cells, e.g. light-reflecting means or light-concentrating means
    • H10F77/48Back surface reflectors [BSR]
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/52PV systems with concentrators
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/545Microcrystalline silicon PV cells
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/548Amorphous silicon PV cells
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50Manufacturing or production processes characterised by the final manufactured product

Landscapes

  • Photovoltaic Devices (AREA)

Abstract

This invention relates to a solar cell arrangement and to a process for manufacturing thin film silicon-based solar cells. It particular addresses the topic of reducing the active layer thicknesses significantly by advanced light trapping. The invention proposes a solar cell arrangement with an extent > 1.4 m<SP>2</SP> in tandem configuration comprising an a-Si Cell (4) and a μ c-Si cell (10), the absorber layer of the a-Si cell (4) having a thickness of 210 nm ± 20 nm, the absorber layer of the μ c-Si cell (10) having a thickness of 900 nm ± 200 nm.

Description

201216491 六、發明說明: 【發明所屬之技術領域】 本發明係關於一種用於製造薄膜矽基太陽能 製程。特別是著眼在藉由先進的光捕捉來顯著減 層厚度的議題。 【先前技術】 光伏打太陽能轉換所提供的觀點在於提供用 電力之%保裝置。然而,在目前的狀態下,藉由 月b篁轉換單元所提供的電能仍顯著較藉由習知之 所k ί、的電力更為昂貴。因此,發展更具成本效 造光伏打能量轉換單元的裝置在近幾年備受關注 造低成本太陽能電池的不同方法之中,薄膜矽太 池結合數種有利的形式:首先,薄膜矽太陽能電 由例如電漿增強化學氣相沈積(PECVD)之已知的 積技術來製備’從而提供協同作用之觀點,以藉 過去在例如其他薄膜沈積技術領域(例如,顯示^ 所獲得的經驗來降低製造成本。其次,薄膜矽太 池可奮力達到1〇%甚至更高的高能量轉換效率。 用於製/專膜;5夕基太陽能電池的主要原料既充足 毒性。 一薄膜太陽能電池通常包括連續堆疊在一基 一第一電極、—或多個半導體薄膜p_i_n或 第一電榼。第1圖顯示一在此技術中已知的串 矽薄膜太陽能電池。這一類薄膜太陽能電池5 0在 41上通常包括一第一或前電極42、一或多個半導 電池之 少主動 來產生 光伏打 發電廠 益之製 。在製 陽能電 池可藉 薄膜沈 由使用 i領域) 陽能電 第三, 又不具 材上的 接面及 接接面 一基材 體薄膜 201216491 p-i-n接面(52-54、5卜44-46、43)及一第二或背電極47。 母Pin接面51、43或薄膜光電轉換單元包括一本質 上固有的i型| 53、45,其係夾在—p型層52、44及 η孓層54 46中間(ρ型=正換雜,11型=負摻雜)。在 此上下文中,「本質上固有」係理解為未經摻雜或實質上 未顯出L雜任·何生成物。光電轉換主要發生在此丨型層 中;因此亦將其稱為「吸收層」。 依…、1型層5 3、4 5的結晶分數(結晶度)而定,太陽 能電池或光電(轉換)裝置的特徵分為非晶(非晶矽 (a-S!),53)或微晶(微晶矽hc_Si),45)太陽能電池,其與 鄰接之P型層及η型層的結晶度種類無關。如常見於: 技術之「微晶」層’其係理解為在—非晶基質中由絕大 部分之結晶矽(所謂的微晶粒)所構成的層。接面之 堆疊稱為串接或三接面光伏打電池。如第工圖所示,一 非晶及微日日日p-i.n接面之組合亦稱為「非微晶串接電 池」。第i圖顯示-先前技術之串接接面薄膜石夕光伏打電 池。其厚度並未按比例繪製。 【發明内容】 懾官便用低厚度,對薄膜石夕太陽能電池而古,主要 的成本因素之-仍是層的厚度(特別是i型層的。厚度卜 例如’對非微晶串接電池而古,與曰γ ^ ^ ^ ^ 5 φ r °碱日日(Μ)底部電池的範 圍常為1.5μιη或甚至更厚。此厚廑 子X在。午多方面均影變到 薄膜太陽能電池之製造者的所有權成本. a 對沈積本身及後續的電漿清潔兩 「 要矽沈積系統(例如’ pecvd)之县制和从 )之長持續時間。.由於 -4- 201216491 處理時間嚴重影響所有 這類製造系統通常是主要投資 權成本。 ~ 另外’用於沈積及清潔的氣體亦具有巨大影響,特 燒SlH4及氣來源氣體(例如,_3、阳脅當 :予度可予以減少時’所有這些因素本質上均可加以縮 減〇 . 發明内容 本發明之一 太陽能電池。 目軚為提供具有減少之層厚度的高性能 此藉由如申請專利範圍第【項所述之太陽能電池裝 置以及如中請專利範圍第8項所述之製造這―類太陽能 電池裝置之方法來達成。本發明進—步的實施例係在申 請專利範圍附屬項中詳細說明。 本發明涉及一種太陽能電池裝置,其串接配置具有 大於1.4 m的面積,且包括一非晶矽(a_si)電池及一微 晶矽(μο-Si)電池,該非晶矽電池之吸收層具有21〇 nm±20 nm之厚度,該微晶矽電池之吸收層具有9〇〇 nm±200 nm之厚度。 為了實現具有減少之層厚度之高性能模組,有兩個 關鍵準則。其一為整片玻璃上方之層的高均勻性,因為 在低的層厚度之下’由光伏打所產生的電流變得對厚产 變動更為敏感’電池更加遠離飽和電流。這樣的話,^ 度的小幅波動可導致大電流差’那樣的 al . m 予 依·的活,則會因電流 限制而降低總效率。此示於第 2 n r ㈢(針對非晶矽進行模 擬)。 、 -5- 201216491 ”::準則為實現良好的光捕捉。「光捕捉」意指太 -電池利用照射光的能力。?文善光捕捉行為的對策為 反射塗層、紋理化或生成態粗糙的tc〇層,另外則是 取例如延伸光在吸收厚Φ &gt; 士 , ' r尤隹及收層中之有效路徑的任何步驟。一 =品的層厚度係藉由兩個因素來決定-光捕捉 在具有良好光捕捉的情況下,能以較低厚度達成 著的光吸收。材料品質的限”U較高厚度無法萃 所產生的電荷載體,因為電荷 載體在抵達電極層之前 ^度Μ。第3圖繪示改善的光捕捉如何使最佳效率 移至較低厚度(亦針對非晶矽進行模擬卜 雖然上文所提及的係顯示為針對非晶石夕, 對例如第1圖所示之非微晶型 言是相同的。 的串接接面太陽能電池 具有工業級高性能薄層 i佔田古认&amp; 心大的太除能模組現今係 由使用同均勾性的沈積設備來製$,例如 (Sw^^ — -t,,, 工具TC〇12〇°及KAI1200。為了最佳的光捕捉,必須 佳化别接觸層與背接觸層之一組人。 、 、σ 名貝夕卜引入一 έ®扑 的背反射器(白箔)。當在薄膜太 守联太%能電池堆疊中散布 反射㈣’此白羯取代白;泰:參見第4圖。 那樣的話,便可在不損耗底部電池之 況下實現厚度:參見第5圖。 〜^ 相抵ί根Ϊ本發明之太陽能電池裝置之-變體中,除 相抵觸’否則可將其與任何欲提出的變體結合,且其 陽 抗 採 般 及 顯 取 便 偏 應 而 藉 士 積 最 善 背 情 非 吸 201216491 收層具有土 5 %之均質性。 何已提出或欲提出之變 之太陽能電池裝置包括 25%的混濁度,且較佳 在除非相抵觸,否則可與任 體結合之一變體中,根據本發明 一 ZnO透明導電氧化層,其具有 的是藉由LPCVD來沈積。 在除非相抵觸’否則可與任何已提出或欲提出之變 體結合之-變體中,根據本發明之太陽能電池裝置包括 -作為ZnO背電極之透明導電氧化層其具有1〇%之混 濁度均質性’且較佳的是藉由LpcvD來沈積。 在除非相抵觸,否則可與任何已提出或欲提出之變 體結合之一變體中,根據本發明之太陽能電池裝置包括 作為为反射器之白羯,較佳的是聚乙稀縮丁酸,較佳 的是配有白反射粒子,且較佳的是具有G 5mm的厚度。 在除非相抵觸,否則可與任何已提出或欲提出之變 體結合之一變體中,根據本發明之太陽能電池裝置具有 小於1 0 %之光誘導劣化。 在除非相抵觸’否則可與任何已提出或欲提出之變 體結合之一根據本發明之太陽能電池裝置的變體中,非 晶石夕電池包括一10 nm的矽P型層、一 210 nm的a_Si : H吸收層、一 30 nm的η塑層,且該微晶矽電池包括— 24 nm的ρ型層、一 9〇〇 nm的με-Si: Η吸收層及一36 nm 的η型層。 本發明進一步包含一種製造太陽能電池裝置的方 法’ e亥太陽能電池裝置串接配置具有一大於的面 積 且包括·一非晶碎電池及一微晶碎電池’該非晶碎電 201216491 池(4)之吸收層具有一 2 1 0 nm±20 nm之厚度’該微晶矽 電池之吸收層具有一 900 nm±200 nm之厚度,且該方法 包含以下步驟: •以下列沈積參數PECVD沈積非晶矽電池之吸 收層:201216491 VI. Description of the Invention: TECHNICAL FIELD OF THE INVENTION The present invention relates to a process for fabricating a thin film germanium-based solar energy. In particular, the issue of significantly reducing the thickness of the layer by advanced light trapping is focused. [Prior Art] The viewpoint provided by photovoltaic solar energy conversion is to provide a % protection device for power consumption. However, in the current state, the power supplied by the monthly b conversion unit is still significantly more expensive than the power of the conventional one. Therefore, in the development of more cost-effective photovoltaic energy conversion unit devices in recent years, the film 矽 Taichi pool combines several advantageous forms: first, the film 矽 solar power The viewpoint of providing a synergistic effect by a known product technique such as plasma enhanced chemical vapor deposition (PECVD) to reduce manufacturing in the past, for example, in the field of other thin film deposition techniques (for example, the experience gained) Cost. Secondly, the film 矽 Taichi can strive to achieve high energy conversion efficiency of 1% or higher. It is used for manufacturing/special film; the main raw materials of the 5th solar cell are both sufficiently toxic. A thin film solar cell usually includes continuous stacking. In a base-first electrode, or a plurality of semiconductor films p_i_n or a first electrode. Figure 1 shows a tandem thin film solar cell known in the art. This type of thin film solar cell 50 is usually at 41. Include a first or front electrode 42 and one or more semi-conductive batteries to actively generate photovoltaic power generation system. The film sink is made of i field. The third is the solar energy, and there is no joint on the material and the joint surface. The substrate film 201216491 pin joint (52-54, 5 Bu 44-46, 43) and a second Or the back electrode 47. The female Pin junction 51, 43 or the thin film photoelectric conversion unit includes an essentially intrinsic i-type | 53, 45 which is sandwiched between the -p-type layers 52, 44 and the η-layer 54 46 (ρ-type = positive-changing) , type 11 = negative doping). In this context, "intrinsically intrinsic" is understood to mean undoped or substantially unexpressed. Photoelectric conversion occurs mainly in this ruthenium layer; therefore, it is also referred to as an "absorption layer." Depending on the crystal fraction (crystallinity) of the type 1 layer 5 3, 4 5 , the characteristics of the solar cell or photoelectric (conversion) device are classified into amorphous (amorphous germanium (aS!), 53) or microcrystalline ( Microcrystalline germanium hc_Si), 45) solar cell, regardless of the crystallinity type of the adjacent P-type layer and the n-type layer. As is common in the "microcrystalline" layer of technology, it is understood to be a layer composed of a majority of crystalline cerium (so-called microcrystalline) in an amorphous matrix. The stack of junctions is called a series or triple junction photovoltaic cell. As shown in the figure, a combination of amorphous and micro-day p-i.n junctions is also referred to as a "non-microcrystalline tandem battery". Figure i shows a prior art tandem junction film lithography photovoltaic cell. Its thickness is not drawn to scale. [Summary of the Invention] Eunuchs use low thickness, the ancient cost of the thin-film solar cell, the main cost factor - still the thickness of the layer (especially the i-type layer. Thickness such as 'for non-microcrystalline tandem battery However, in ancient times, the range of the bottom cell of 曰γ ^ ^ ^ ^ 5 φ r ° alkali is usually 1.5 μιηη or even thicker. This thick scorpion X is changed to thin film solar cells in many aspects. The cost of ownership of the manufacturer. a. The duration of the deposition itself and subsequent plasma cleaning. The duration of the sedimentation system (eg, 'pecvd') is long. Since -4- 201216491 processing time seriously affects all This kind of manufacturing system is usually the main investment cost. ~ In addition, the gas used for deposition and cleaning also has a huge impact. Specially burned SlH4 and gas source gas (for example, _3, Yangwon: When the degree can be reduced) The present invention is a solar cell of the present invention. It is a solar cell device of the present invention. The method for manufacturing the solar cell device according to the eighth aspect of the patent is to be achieved. The further embodiments of the present invention are described in detail in the appended claims. The present invention relates to a solar cell device. The tandem configuration has an area greater than 1.4 m and includes an amorphous germanium (a_si) battery and a microcrystalline germanium (μο-Si) battery, the amorphous germanium battery having an absorber layer having a thickness of 21 〇 nm ± 20 nm. The absorption layer of the microcrystalline germanium battery has a thickness of 9 〇〇 nm ± 200 nm. In order to realize a high performance module with reduced layer thickness, there are two key criteria. One is the high uniformity of the layer above the entire glass. Sex, because at low layer thicknesses, the current generated by photovoltaics becomes more sensitive to changes in the yield. The battery is farther away from the saturation current. In this case, small fluctuations in the ^ can cause large current differences. Al. m The activity of yue will reduce the total efficiency due to current limitation. This is shown in the 2nd nr (3) (simulation for amorphous yttrium). , -5- 201216491 ”:: Guidelines for achieving good light trapping " "Capture" means too - the ability of the battery to illuminate the light. The countermeasures for Wen Shanguang's capture behavior are reflective coating, texturing or rough-formed tc〇 layer, and in addition, for example, extending light at absorption thickness Φ &gt; , ' r 隹 and any step of the effective path in the layer. The layer thickness of a product is determined by two factors - light capture can be achieved with a low thickness in the case of good light trapping Light absorption. The limit of material quality "U high thickness can not extract the generated charge carriers, because the charge carriers before the arrival of the electrode layer ^ Figure. Figure 3 shows how improved light capture to make the best efficiency to lower The thickness (also simulated for amorphous bismuth) although the above-mentioned series is shown to be for amorphous, is the same for the non-microcrystalline type shown in Fig. 1, for example. The tandem junction solar cell has an industrial-grade high-performance thin layer i. Zhan Tian Gu &amp; The big de-energy module is now made by using the same homogenous deposition equipment, for example (Sw ^ ^ - -t,,, Tools TC〇12〇° and KAI1200. For the best light capture, one of the contact layer and the back contact layer must be better. 、, σ名贝布 Introduces a έ® flap back Reflector (white foil). Disperse reflection when the film is too defensive. (4) 'This white plaque replaces white; Thai: See Figure 4. In that case, the thickness can be achieved without loss of the bottom battery. See Fig. 5. ~ 相 ί Ϊ 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能 太阳能It is the best and the best, and the non-absorbable 201216491 layer has a homogeneity of 5%. The solar cell device that has been proposed or proposed to change includes 25% turbidity, and preferably unless it contradicts, Otherwise a variant that can be combined with any of the bodies, according to the invention a ZnO transparent conductive oxide layer having a deposition by LPCVD. The solar cell device according to the present invention includes - as a variant, which can be combined with any variant proposed or proposed, unless it is inconsistent The transparent conductive oxide layer of the ZnO back electrode has a turbidity homogeneity of 1% and is preferably deposited by LpcvD. It can be combined with any variant proposed or proposed, unless otherwise contradicted. In a variant, the solar cell device according to the invention comprises, as a reflector, a white crucible, preferably a poly(butyric acid), preferably with white reflective particles, and preferably having a G 5 mm Thickness. A solar cell device according to the present invention has less than 100% light-induced degradation in addition to any variant that has been proposed or proposed to be combined, unless otherwise contradicted. In a variant of the solar cell device according to the invention in combination with any variant proposed or intended to be modified, the amorphous Austenitic battery comprises a 10 nm 矽P-type layer, a 210 nm a_Si:H absorbing layer, a 30 nm η plastic layer, and the microcrystalline germanium battery includes a 24 nm p-type layer, a 9 μm με-Si: germanium absorption layer, and a 36 nm n-type layer. The present invention further includes a fabrication The solar cell device method 'Ehai solar cell device serial configuration has a larger area and includes an amorphous crushed battery and a microcrystalline broken battery'. The amorphous crushed 201216491 pool (4) has an absorption layer of 2 1 0 nm ± 20 nm thickness The absorption layer of the microcrystalline germanium battery has a thickness of 900 nm ± 200 nm, and the method comprises the following steps: • depositing an absorber layer of an amorphous germanium battery by PECVD with the following deposition parameters:

• SiH4的流量:10.4 slm •H2的流量:10.4 slm •沈積速率:3.35人/s •沈積時間:6 3 4秒 •壓力:0.5 mbar •溫度:2 0 〇0 C •功率:380 W ;及 -以下列沈積參數PECVD沈積微晶矽電池之吸 收層: • SiH4的流量:7.7 slm • H2的流量:17〇 slm •沈積速率:5A/S •沈積時間:1 8 3 0秒 •壓力.2.5 mbar •溫度:160 °C •功率:3500 W。 在除非相抵觸,否則可與任何欲提出之變體結合之 一根據本發明之方法的變體中,該裝置進一步包括一具 有25%之混濁度的Zn〇透明導電氧化層,並包含以下列 沈積參數LPCVD沈積該Zn〇層: 201216491• Flow rate of SiH4: 10.4 slm • Flow rate of H2: 10.4 slm • Deposition rate: 3.35 person/s • Deposition time: 6 3 4 seconds • Pressure: 0.5 mbar • Temperature: 2 0 〇0 C • Power: 380 W; - The absorption layer of the microcrystalline germanium battery was deposited by PECVD with the following deposition parameters: • Flow rate of SiH4: 7.7 slm • Flow rate of H2: 17〇slm • Deposition rate: 5A/S • Deposition time: 1 8 3 0 seconds • Pressure. 2.5 Barr • Temperature: 160 °C • Power: 3500 W. In a variant of the method according to the invention, which may be combined with any variant to be proposed, unless otherwise contradicted, the apparatus further comprises a Zn〇 transparent conductive oxide layer having a haze of 25% and comprising the following Deposition of the parameters LPCVD deposition of the Zn layer: 201216491

•溫度.:1 8 0 °C • H2的流量:577 seem • B2H6的流量:400 seem • Η2〇的流量:2460 seem •DEZ的流量:2200 seem •壓力:Ο · 5 mbar。 在除非相抵觸,否則可與任何已提出或欲提出之變 體結合之一變體中,根據本發明之方法,該非晶矽電池 包括一 10nm的石夕p型層、一 210ηηι的a-Si:H吸收層、 一 30nm的η型層,該微晶石夕電池包括一 24nm的p型 層、一 900nm的pc-Si:H吸收層及一 36nm的η型層, 且該方法包含以下步驟: -以下列沈積參數沈積非晶矽電池之ρ型層: • SiHU的流量:5.64 slm • Η 2 的流量:1 0 · 5 8 s 1 m 。 •三曱棚(TMB)的流量:6.45 slm• Temperature.: 1 8 0 °C • Flow of H2: 577 seem • Flow of B2H6: 400 seem • Flow of Η2〇: 2460 seem • Flow of DEZ: 2200 seem • Pressure: Ο · 5 mbar. In a variant that can be combined with any variant proposed or proposed, unless otherwise contradicted, the amorphous tantalum cell comprises a 10 nm Shi Xi p-type layer, a 210 nη a-Si, in accordance with the method of the present invention. : a H-absorbing layer, a 30 nm n-type layer, the microcrystalline cell comprises a 24 nm p-type layer, a 900 nm pc-Si:H absorption layer and a 36 nm n-type layer, and the method comprises the following steps : - Deposition of the p-type layer of an amorphous tantalum battery with the following deposition parameters: • Flow rate of SiHU: 5.64 slm • Flow of Η 2: 1 0 · 5 8 s 1 m. • Three sheds (TMB) flow: 6.45 slm

• C Η 4 的流量:1 0.2 6 s 1 m •沈積速率:2.6 A/s •沈積時間:39秒 •壓力:0.5 mbar •溫度:200 °C •功率:295 W ; -以下列沈積參數沈積非晶矽電池之η型層: • SiH4的流量:0.86 slm • Η 2的流量:9 5 s 1 m 201216491• Flow rate of C Η 4: 1 0.2 6 s 1 m • Deposition rate: 2.6 A/s • Deposition time: 39 seconds • Pressure: 0.5 mbar • Temperature: 200 °C • Power: 295 W; - Deposition with the following deposition parameters The n-type layer of the amorphous germanium battery: • Flow of SiH4: 0.86 slm • Flow of Η 2: 9 5 s 1 m 201216491

• Ρ Η 3 的流量:1.0 2 s 1 m •沈積速率:1 A/s •沈積時間:300秒 •壓力:2 mbar •溫度:200 °C •功率:1 800 W ; -以下列沈積參數沈積微晶矽電池之ρ型層: • S i Η 4 的流量:1.6 s 1 m • Η 2 的流量:2 0 0 s 1 m •三甲石朋(TMB)的流量:0.5slm •沈積速率:1.4 A/s •沈積時間:1 7 5秒 •壓力:2.5 mb ar• Flow rate of Ρ Η 3: 1.0 2 s 1 m • Deposition rate: 1 A/s • Deposition time: 300 sec • Pressure: 2 mbar • Temperature: 200 °C • Power: 1 800 W; - Deposition with the following deposition parameters The p-type layer of the microcrystalline germanium battery: • Flow of S i Η 4: 1.6 s 1 m • Flow of Η 2 : 2 0 0 s 1 m • Flow of trimethoate (TMB): 0.5 slm • Deposition rate: 1.4 A/s • Deposition time: 1 7 5 seconds • Pressure: 2.5 mb ar

•溫度:160 °C •功率:3100 W ;及 -以下列沈積參數沈積微晶矽電池之η型層: • SiH4的流量:6.21 slm • Η 2 的流量:1 4.3 6 s 1 m • Ρ Η 3的流量:4 s 1 m •沈積速率:2 A/s •沈積時間:180秒 •壓力:〇_5 mbar •溫度:160 °C •功率:700 W。 在除非相抵觸,否則可與任何已提出或欲提出之變 -10- 201216491 體結合之一根據本發 型層之沈積與該吸收層^ϊ變體中’該方法在該p 理。 u積間包含一水蒸氣沖洗處 在除非相抵觸,否則 體結合之一變辦由 、j j與任何已提出或欲提出之變 處理传在U0 f ,根據本發明之方法,該水蒸氣沖洗 地埋係在120秒期間 A ^ 4 ^ mbar的蒸氣壓力執行。 在除非相抵觸,否則 體結合之一變體中攄:壬何已提出或欲提出之變 電、、也之1 ^ 根據本發明之方法,介於該非晶矽 电池之该ρ型層與該 7 理仫户《 席之沈積間的該水蒸氣沖洗處 理係在120秒期間以2 mbar沾# 处 妈曰 的裘氣壓力執行,且介於該 微晶矽之該p型層與該吸 ^ ^ TS r.. 日之沈積間的該水蒸氣沖洗 處理係在120秒期間以丨 T无 【實施方式】 · 的蒸氣壓力執行。 本發明須在圖式之協助下作出進一步的例示。 第i圖顯示先前技術之串接接面薄膜猶 5〇(厚度未按比例繪製)^箭 &gt; ^ 11貝才日不照射光的方向。該串 接接面包括基材41、前電極42、底部電池43、p型摻雜 矽層(p μο-Si . H) 44、i 型屛 ’、 土增pc-Si : η 45、η型摻雜石々 層(n a-Si : H/n μο-Si : Η) 46、呰带 * 、身電極47、背反射器48、 頂部電池5卜P型摻雜石夕層(…ι:Η/ρ — :Η)52、 1 型層 a-Si : Η 53、n 型摻雜矽層(n a_si : H/n :• Temperature: 160 °C • Power: 3100 W; and - The n-type layer of the microcrystalline germanium battery is deposited with the following deposition parameters: • Flow of SiH4: 6.21 slm • Flow of Η 2: 1 4.3 6 s 1 m • Ρ Η Flow rate of 3: 4 s 1 m • Deposition rate: 2 A/s • Deposition time: 180 seconds • Pressure: 〇_5 mbar • Temperature: 160 °C • Power: 700 W. Unless otherwise contradicted, it may be combined with any of the proposed or proposed changes -10-201216491 in accordance with the deposition of the hairline layer and the absorbing layer. The u-product contains a water vapor flushing device unless it is inconsistent, otherwise one of the body bonds is changed, jj and any proposed or proposed variable process is transmitted to U0f, according to the method of the present invention, the water vapor flushing The buried system is carried out at a vapor pressure of A ^ 4 ^ mbar during 120 seconds. Unless there is a contradiction, otherwise a variant of the body is combined with: a transformation that has been proposed or proposed, and 1 ^ according to the method of the invention, the p-type layer between the amorphous tantalum battery and the 7 The housekeeper's “steam flushing process between the sediments of the mat is performed during the 120 seconds with the helium pressure of the 2 mbar ##, and the p-type layer between the microcrystalline 与 and the absorbing ^ ^ TS r.. The steam rinsing treatment between the sediments of the day is performed at a vapor pressure of 丨T without [Embodiment] during 120 seconds. The invention is further illustrated with the aid of the drawings. The figure i shows that the prior art tandem junction film is still 5 (thickness is not drawn to scale) ^ arrow &gt; ^ 11 is the direction in which the light is not illuminated. The series connection surface comprises a substrate 41, a front electrode 42, a bottom cell 43, a p-type doped germanium layer (p μο-Si. H) 44, an i-type 屛', a soil-enhanced pc-Si: η 45, an n-type Doped sarcophagus layer (n a-Si : H/n μο-Si : Η) 46, 呰 band*, body electrode 47, back reflector 48, top cell 5 P-type doped layer (... ι: Η/ρ — :Η) 52, type 1 layer a-Si : Η 53, n-type doped yttrium layer (n a_si : H/n :

54。 J 第6圖顯示根據本發明之一串接接面,其為所謂的 非微晶堆疊(miCr〇morph)接面形式。該串接接面包=具 有1_55 μηι厚度的前接觸層3、具有21〇nm厚度的非晶 201216491 矽層4、具有900 nm厚度的pC-Si:H層1〇、具有! 55 μιη 厚度的背接觸層1 1及白箔1 3 » 本發明藉由下列方式提出一用於在大於i 4 m2的大 面積上於高穩定功率下製造具有減少之吸收層厚度之薄 膜電池的方法: a) 利用高度均質之高混濁度前接觸層在整個沈積面 積上方增強光捕捉能力;及 b) 將一具有改善之反射性質的白箔用作背反射器; c) 藉由增加半導體層的均質性來降低該層之厚度差 的效應;及 d) 藉由減少矽層之厚度從而降低對非晶矽劣化的 感性。 在第1圖所示之串接接面配置中的吸收層(丨型層 3 45)對頂部電池S1而言可減少至_土2〇 nm,且 對底。卩包池43而言可減少至9〇〇±200 nm。此可在不損 穩定力率的情況下達成。在先前技術中,所實現的頂 部電池5 1 i古&amp; 1 Λ Λ 有約300 nm的厚度,且底部電池43約為 小4 5 μιη。在本發明的協助之下,對頂部電池而言,可減 ^ 1 /3的材料成本與時間。底部電池的厚度幾乎可減少 !此實皙ρ β m 乂 貝上疋因為(i)在太陽能面板之主動零件中,半 V體層之均曾μ 負性改善至+-5% ;及(ii)LPCVD ΖηΟ層之均 質性改善至丨〇 0/ U /〇 /昆濁度均勻性;及(iii)25 %的高混濁度。 所有這些成就#也s , 。。 Λ就徒供良好的光偈限或光捕捉。作為背反射 裔層48的白嚅接 ,白徒供極為良好的背反射,且光散射因此進 —步地有助於_ '艮好的光侷限。改善的反射提供更多光給 201216491 頂部電池,從而使更薄的電池成為可能。 另一要點為較薄的頂部電池(非晶矽)呈現較低的劣 化(Staebler-Wr〇nski效應)。藉此使串接接面電池的總劣 化顯著降低到低於1 0 %。 藉由p型層及i型層間之改善的處理(1 2 mbar持續 1 2 0秒的水蒸氣沖洗)來改善底部電池的品質。底部電池 的性能增強,改善的光捕捉提供非常薄的電池。 八有根據第1圖之結構並具有根據本發明之優點的 電池包括M LPCVD ZnQ t成的前電極42、來自石夕的 Ρΐη_Ρ1Γ1頂部/底部電池結構及以LPCVD Zn〇製成的背電 極47 ’其後則是白羯反射器。此白落較佳的是配有白反 射粒子或其均等物之聚乙烯縮丁醛箔。前42電極具有 + /-10%之均質性之25%的平均混濁度。 ^!ATC0沈積工具之改善的負載鎖定系統來幫助 、&quot;捕捉。該負載鎖定的相關 中敘述,其係以參照的方式:二在二s 係 C的負載鎖定溫度、2〇〇SCcmtB2 2〇〇 seem 之 DEZ(二乙基鋅 6〇sc : 的梦 if ® γ 又 H2〇 在 0.5 mbar 、 下進行沈積。該p i n結構所 且右1 η , 丹W呈現的頂部電池 、 nm的矽P型層、2 1 0 nm的i型声( nm的η型層 ^ ♦ 孓層UA : Η)、30 主增。底部電池呈現24 nm的η刑Μ 的固有矽^ 妁Ρ型層、900 nm ’ 7 (gc-Sl : H)層及最終之36 _的 層的厚产矣t 的n型層。吸收 …子度差如上文所提及,p型層 + /-20%。 土增的厚度差為 -13- 201216491 之間執行水蒸氣處理(水沖洗)。該製程在US 7,504,279 提出,因而將該揭示内容以參照的方式併入於此。針對 第一 p-i接面的蒸氣壓力為2 mbar持續120秒。在第二 p-i介面的壓力是1.2 mbar持續120秒。pin矽結構之後 為藉由LPCVD製造的TCO ZnO背電極47。沈積參數如 下:負載鎖定溫度 180t:、H2 577sccm、B2H6400sccm、 H2O 2460 seem、DEZ 2200 seem、製程壓力 0.5 mbar。 整個堆疊終止於厚度0.5 mm的白箔。 表154. J Figure 6 shows a series of junctions in accordance with the present invention in the form of a so-called non-microcrystalline stack (miCr〇morph) junction. The tandem bread = front contact layer 3 having a thickness of 1_55 μηι, amorphous 201216491 tantalum layer 4 having a thickness of 21 〇 nm, pC-Si:H layer having a thickness of 900 nm, having! 55 μιη thickness of back contact layer 1 1 and white foil 1 3 » The present invention proposes a method for producing a thin film battery having a reduced absorption layer thickness at a high stable power over a large area of more than i 4 m 2 in the following manner Method: a) using a highly homogeneous high turbidity front contact layer to enhance light capture capability over the entire deposition area; and b) using a white foil with improved reflective properties as a back reflector; c) by adding a semiconductor layer Homogenization to reduce the effect of the thickness difference of the layer; and d) to reduce the sensitivity to the degradation of the amorphous ruthenium by reducing the thickness of the ruthenium layer. The absorbing layer (丨-type layer 3 45) in the series connection configuration shown in Fig. 1 can be reduced to _ soil 2 〇 nm and to the bottom for the top battery S1. In the case of the bag pool 43, it can be reduced to 9 〇〇 ± 200 nm. This can be achieved without compromising the rate of stability. In the prior art, the top cell 5 1 i &amp; 1 Λ 实现 achieved has a thickness of about 300 nm, and the bottom cell 43 is about 45 μm. With the aid of the present invention, the material cost and time can be reduced by a factor of 1/3 for the top battery. The thickness of the bottom battery can be reduced almost! This 皙ρ β m 乂 疋 疋 because (i) in the active parts of the solar panel, the half V body layer has been negatively negative to +-5%; and (ii) The homogeneity of the LPCVD Ζη layer was improved to 丨〇0/U /〇/kun turbidity uniformity; and (iii) 25% high turbidity. All these achievements #also s, . . You can use a good light limit or light capture. As a white-backed layer of the back-reflective layer 48, the whites provide excellent back reflections, and light scattering thus contributes to the _ 'good light limitation. The improved reflection provides more light to the 201216491 top battery, making thinner batteries possible. Another point is that the thinner top cell (amorphous germanium) exhibits a lower degradation (Staebler-Wr〇nski effect). Thereby, the total deterioration of the tandem junction battery is significantly reduced to less than 10%. The quality of the bottom cell is improved by an improved treatment between the p-type layer and the i-type layer (1 2 mbar for a water vapor rinse of 120 seconds). The performance of the bottom battery is enhanced and the improved light capture provides a very thin battery. 8. A battery having the structure according to Fig. 1 and having advantages according to the present invention comprises a front electrode 42 made of M LPCVD ZnQ t , a top/bottom cell structure of Ρΐη_Ρ1Γ1 from Shi Xi, and a back electrode 47 ' made of LPCVD Zn〇. This is followed by a chalk reflector. Preferably, the white fall is a polyvinyl butyral foil provided with white reflective particles or equivalents thereof. The first 42 electrodes have an average haze of 25% of the homogeneity of + /-10%. ^! ATC0 Deposition Tool's improved load-locking system to help, &&quot;capture. The relevant description of the load lock is described in the following manner: two at the load lock temperature of the second s system C, 2 〇〇SCcmtB2 2〇〇seem DEZ (diethylzinc 6〇sc: dream if γ H2〇 is deposited at 0.5 mbar. The pin structure is 1 η right, the top cell of Dan W, the 矽P-type layer of nm, and the i-type sound of 2 10 nm (n-type layer of nm ^ ♦孓 layer UA: Η), 30 main increase. The bottom cell presents an inherent 矽^ 妁Ρ layer of 24 nm η Μ , 900 nm ' 7 (gc-Sl : H) layer and the thickness of the final 36 _ layer The n-type layer of 矣t. The absorption difference is as mentioned above, p-type layer + / -20%. The difference in soil thickness is between -13 and 201216491, and steam treatment (water rinsing) is performed. The process is set forth in US Pat. No. 7,504,279, the disclosure of which is hereby incorporated herein by reference in its entirety in its entirety in the the the the the the the the the Second, the pin矽 structure is followed by a TCO ZnO back electrode 47 fabricated by LPCVD. The deposition parameters are as follows: load lock temperature 180t: H2 577sccm, B2H6400sccm , H2O 2460 seem, DEZ 2200 seem, process pressure 0.5 mbar. The entire stack is terminated by a white foil with a thickness of 0.5 mm.

SiH4 slm h2 slm TMB slm ph3 slm ch4 slm DR A/s Dep t s 壓力 mbar 溫度 Dep °c 功率 瓦特 P _5.64 10.58 6.45 10.26 2.6 39 0.5 200 295 I -' — 10.4 ——— 10.4 3.35 634 0.5 200 380 N — — __0.86 95 1.02 1 300 2 200 1800 P -- 1.6 200 0.5 1.41 175 2.5 160 3100 I 7.7 170 5 1830 2.5 160 3500 N 6.21 L--- 14.36 4 2 180 0.5 160 — 700 TMB =三甲硼、DR=沈積速率、Dep t =沈積時間,所 有給定值係適用於欲塗佈之1.4m2基材。 所述之層的順序係如第1圖所示及所沈積者。 【圖式簡單說明】 第1圖:根據先前技術之一串接接面薄膜矽光伏打 電池的圖; 第2圖:繪示與i型層厚度相關之Jsc的圖; 第3圖:繪示與厚度相關之穩定Eta的圖; 第4圖:緣示與波長相關之總反射比的圖; -14- 201216491 第5圖:繪示與底部電池厚度相關之P m p p的圖 第6圖 :根據本發明之一串接接面的圖’ 【主要元件符號說明】 3 前接觸層 4 非晶矽層 10 pc-Si : Η 層 11 背接觸層 13 白f各 41 基材 42 前電極 43 底部電池 44 p型層 45 i型層 46 η型層 47 背電極 48 背反射器 50 串接接面薄膜矽光伏打電池 51 頂部電池 52 Ρ型層 53 i型層 54 η型層SiH4 slm h2 slm TMB slm ph3 slm ch4 slm DR A/s Dep ts Pressure mbar Temperature Dep °c Power watt P _5.64 10.58 6.45 10.26 2.6 39 0.5 200 295 I -' — 10.4 ——— 10.4 3.35 634 0.5 200 380 N — — __0.86 95 1.02 1 300 2 200 1800 P -- 1.6 200 0.5 1.41 175 2.5 160 3100 I 7.7 170 5 1830 2.5 160 3500 N 6.21 L--- 14.36 4 2 180 0.5 160 — 700 TMB = trimethylboron , DR = deposition rate, Dep t = deposition time, all given values apply to the 1.4 m2 substrate to be coated. The order of the layers is as shown in Figure 1 and deposited. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a view showing a tandem junction film 矽 photovoltaic cell according to one of the prior art; FIG. 2: a diagram showing Jsc related to the thickness of the i-type layer; FIG. 3: A graph of the thickness-dependent stable Eta; Figure 4: A plot of the total reflectance associated with the wavelength; -14- 201216491 Figure 5: A diagram showing the P mpp associated with the thickness of the bottom cell. Figure 6: Figure 1 of a series connection of the present invention [Description of main components] 3 front contact layer 4 amorphous germanium layer 10 pc-Si: germanium layer 11 back contact layer 13 white f each 41 substrate 42 front electrode 43 bottom battery 44 p-type layer 45 i-type layer 46 n-type layer 47 back electrode 48 back reflector 50 series junction film 矽 photovoltaic cell 51 top cell 52 Ρ type layer 53 i-type layer 54 η-type layer

Claims (1)

201216491 七、申請專利範圍: 1. 一種太陽能電池裝置,其串接配置具有一大於1.4 m2 的面積,且包括一非晶矽(a-Si)電池及一微晶矽 (pc-Si)電池(1〇) ’該非晶矽電池(4)之該吸收層具有— 210 nm±20 nm之厚度,該微晶矽電池(10)之該吸收層 具有一 900 nm±200 nm之厚度。 2. 如申請專利範圍第丨項所述之太陽能電池裝置,該吸 收層具有±5 %的均質性。 3 _如申請專利範圍第丨或2項所述之太陽能電池裝置,其 包括一 ZnO透明導電氧化層(3),其具有25%之混濁 度’且較佳的是藉由LPCVD來洗積。 4.如申請專利範圍第丨至3項中任一項所述之太陽能電 池裝置,其包括作為一 Zn0背電極之一透明導電氧化 層(11),其具有1〇%之混濁度均質性且較佳的是藉 由LPCVD來沈積。 9 5·如申請專利範圍第!至4項中任—項所述之太陽能電 池裝置,其包括作為一背反射器之—白箔(13),較佳 的是聚乙烯縮丁醛白箔,較佳的是配有白反射粒子, 且較佳的疋具有0.5 mm的厚度。 6. 如申請專利範圍第!至5項中任—項所述之太陽能電 池裝置’其具有—小於1〇%之光誘導劣化。 7. 如申請專利範圍第〗至6項中任一項所述之太陽能電 池裝置,其中該非晶石夕電池⑷包括—i〇.nm的石夕p型 層、一210 nn^a_si: H吸收層、—3〇 1^的11型層, 且該微晶矽電池(1〇)包括一24 n_p型層、一_職 201216491 的pc-Si: Η吸收層及一 36nm的η型層。 8. —種製造一太陽能電池裝置的方法,該太陽能電池裝 置之串接配置具有一大於1.4 m2的面積,且包括一非 晶矽電池(4)及一微晶矽電池(1 0),該非晶矽電池(4) 之該吸收層具有一 210 nm±20 nm之厚度,該微晶矽電 池(10)之該吸收層具有一 900 nm 土 200 nm之厚度,且該 方法包含以下步驟: -以下列沈積參數PECVD沈積該非晶矽電池(4) 之該吸收層: • S i Η 4 的流量:1 0.4 s 1 m • Η 2 的流量:1 0.4 s 1 m • 沈積速率:3.35 A/s • 沈積時間·· 6 3 4秒 •壓力:0 _ 5 mb ar •溫度:200 °C • 功率:380 W ;及 -以下列沈積參數PEC VD沈積該微晶矽電池(1 0) 之該吸收層: • S i Η 4 的流量:7.7 s 1 m • Η 2 的流量:1 7 0 s 1 m • 沈積速率·· 5 A/s • 沈積時間:1 830秒 •壓力:2.5 mb ar •溫度:160 °C •功率:3500 W。 201216491 9.如申請專利範圍第8項所述之方法,其中該裝置進 步包括一具有25%之混濁度的ZnO透明導電氧化層 (3),且該方法包含以下列沈積參數LPCVD沈積該Zn0 層: • 溫度:180°C • H2的流量:577 seem • B2H6的流量:400 seem • H20 的流量:2460 seem • DEZ的流量:2200 seem •壓力·· 〇.5mbar。 1 〇.如申請專利範圍第8或9項所述之方法,其中該非晶矽 電池(4)包括一 1〇 nm的矽p型層、一 210 nm的a-Si : Η 吸收層、一 3 0 n m的η型層,該微晶石夕電池(1 〇)包括一 24 nm的ρ型層、一 900 nm的pc-Si : Η吸收層及-36 nm 的η塑層’且該方法包含以下步驟:-以下列沈積表數 沈積該非晶矽電池(4)之該ρ型層: • SiH4的流量:5.64 slm • H2的流量:10.58 slm •三甲硼(TMB)的流量:6.45 slm • CH4的流量:10.26 slm • 沈積速率:2.6 A/s • 沈積時間:3 9秒 •壓力:0.5 mbar •溫度:200 °C •功率:295 W ; 201216491 -以下列沈積參數沈積該非晶矽電池(4)之該η型 層: • S i Η 4 的流量·_ 0.8 6 s 1 m • Η 2的流量:9 5 s 1 m • Ρ Η 3 的流量:1.0 2 s 1 m • 沈積速率:1人/s • 沈積時間:300秒 •壓力:2 mbar •溫度:200 °C . 功率:1 8 0 0 W ;-以下列沈積參數沈積該 微晶矽電池(1 0)之該ρ型層: • S i Η 4 的流量:1.6 s 1 m • Η 2 的流量:2 0 0 s 1 m • 三曱蝴(TMB)的流量:0.5slm • 沈積速率:1.4 A/s • 沈積時間:1 7 5秒 •壓力:2.5 mbar •溫度:160 °C • 功率:3100 W ;及 -以下列沈積參數沈積該微晶矽電池(10)之該η型 層: • SiH4的流量:6.21 slm • Η 2 的流量·· 1 4 · 3 6 s 1 m • Ρ Η 3的流量:4 s 1 m • 沈積速率:2 A/s -19- 201216491 • 沈積時間:180秒 •壓力:0.5 mbar •溫度:160 °C •功率:700 W。 11.如申請專利範圍第8至1 0項中任一項所述之 在該p型層之沈積與該吸收層之沈積間包含 沖洗處理。 . 1 2.如申請專利範圍第1 1項所述之方法,其中該 洗處理係在120秒期間以1.2 mbar的蒸氣壓力 1 3 ·如申請專利範圍第11項所述之方法,其中 晶矽電池(4)之該p型層與該吸收層之沈積 蒸氣沖洗處理係在1 20秒期間以2 mbar的蒸 行,且藉於該微晶矽(10)之該p型層與該吸 積間的該水蒸氣沖洗處理係在1 20秒其間以 的蒸氣壓力執行。 方法,其 一水蒸氣 水蒸氣沖 執行。 介於該非 間的該水 氣壓力執 收層之沈 1.2 mbar -20-201216491 VII. Patent application scope: 1. A solar cell device having a serial arrangement having an area greater than 1.4 m2 and comprising an amorphous germanium (a-Si) battery and a microcrystalline germanium (pc-Si) battery ( 1)) The absorbing layer of the amorphous bismuth battery (4) has a thickness of -210 nm ± 20 nm, and the absorbing layer of the microcrystalline germanium battery (10) has a thickness of 900 nm ± 200 nm. 2. The solar cell device of claim 2, wherein the absorbing layer has a homogeneity of ± 5%. The solar cell device of claim 2, wherein the ZnO transparent conductive oxide layer (3) has a haze of 25% and is preferably washed by LPCVD. 4. The solar cell device according to any one of claims 3 to 3, comprising a transparent conductive oxide layer (11) as a Zn0 back electrode, having a turbidity homogeneity of 1% It is preferably deposited by LPCVD. 9 5·If you apply for a patent scope! The solar cell device according to any one of the preceding claims, comprising a white foil (13) as a back reflector, preferably a polyvinyl butyral white foil, preferably with white reflective particles. And the preferred crucible has a thickness of 0.5 mm. 6. If you apply for a patent scope! The solar battery device described in any one of the items 5 has a light-induced deterioration of less than 1%. 7. The solar cell device according to any one of claims 1-6, wherein the amorphous radiant battery (4) comprises a stone-like p-type layer of -i〇.nm, a 210 nn^a_si: H absorption The layer, the type 11 layer of -3〇1^, and the microcrystalline germanium battery (1〇) comprises a 24 n_p type layer, a pc-Si of 201216491: a germanium absorption layer and a 36 nm n type layer. 8. A method of fabricating a solar cell device having a tandem configuration having an area greater than 1.4 m2 and comprising an amorphous tantalum cell (4) and a microcrystalline germanium cell (10), the non- The absorbing layer of the wafer battery (4) has a thickness of 210 nm ± 20 nm, and the absorbing layer of the microcrystalline germanium battery (10) has a thickness of 900 nm and a thickness of 200 nm, and the method comprises the following steps: The absorption layer of the amorphous tantalum battery (4) was deposited by PECVD with the following deposition parameters: • Flow rate of S i Η 4: 1 0.4 s 1 m • Flow rate of Η 2 : 1 0.4 s 1 m • Deposition rate: 3.35 A/s • Deposition time · · 6 3 4 sec • Pressure: 0 _ 5 mb ar • Temperature: 200 ° C • Power: 380 W ; and - The absorption of the microcrystalline germanium battery (1 0) is deposited with the following deposition parameters PEC VD Layer: • Flow of S i Η 4: 7.7 s 1 m • Flow of Η 2: 1 7 0 s 1 m • Deposition rate · · 5 A/s • Deposition time: 1 830 seconds • Pressure: 2.5 mb ar • Temperature : 160 °C • Power: 3500 W. The method of claim 8, wherein the device advance comprises a ZnO transparent conductive oxide layer (3) having a haze of 25%, and the method comprises depositing the Zn0 layer by LPCVD with the following deposition parameters. : • Temperature: 180°C • Flow of H2: 577 seem • Flow of B2H6: 400 seem • Flow of H20: 2460 seem • Flow of DEZ: 2200 seem • Pressure · · 〇.5 mbar. The method of claim 8 or claim 9, wherein the amorphous germanium battery (4) comprises a 1 〇 nm 矽p-type layer, a 210 nm a-Si: Η absorption layer, and a 3 An n-type layer of 0 nm, the microcrystalline cell (1 〇) includes a p-type layer of 24 nm, a pc-Si of 900 nm: a ytterbium absorption layer and a -36 nm η plastic layer' and the method comprises The following steps: - depositing the p-type layer of the amorphous tantalum battery (4) with the following number of deposition tables: • Flow rate of SiH4: 5.64 slm • Flow rate of H2: 10.58 slm • Flow rate of trimethylboron (TMB): 6.45 slm • CH4 Flow rate: 10.26 slm • Deposition rate: 2.6 A/s • Deposition time: 3 9 seconds • Pressure: 0.5 mbar • Temperature: 200 °C • Power: 295 W; 201216491 - Deposition of the amorphous tantalum battery with the following deposition parameters (4 The n-type layer: • Flow rate of S i Η 4 · _ 0.8 6 s 1 m • Flow rate of Η 2: 9 5 s 1 m • Flow rate of Ρ Η 3: 1.0 2 s 1 m • Deposition rate: 1 person /s • Deposition time: 300 seconds • Pressure: 2 mbar • Temperature: 200 ° C. Power: 1 800 W; - Deposition of the microcrystalline germanium battery with the following deposition parameters (1 0) of the p-type layer: • Flow rate of S i Η 4: 1.6 s 1 m • Flow rate of Η 2: 2 0 0 s 1 m • Flow rate of triammonium (TMB): 0.5 slm • Deposition rate: 1.4 A/s • Deposition time: 1 7 5 seconds • Pressure: 2.5 mbar • Temperature: 160 °C • Power: 3100 W; and - Deposit the n-type layer of the microcrystalline germanium battery (10) with the following deposition parameters: • Flow rate of SiH4: 6.21 slm • Flow rate of Η 2 · · 1 4 · 3 6 s 1 m • Flow rate of Ρ Η 3: 4 s 1 m • Deposition rate: 2 A/s -19- 201216491 • Deposition time: 180 Seconds • Pressure: 0.5 mbar • Temperature: 160 °C • Power: 700 W. 11. The rinsing treatment is included between the deposition of the p-type layer and the deposition of the absorbing layer as described in any one of claims 8 to 10. The method of claim 11, wherein the washing treatment is carried out at a vapor pressure of 1.2 mbar during a period of 120 seconds. The method of claim 11, wherein the crystal crucible The deposition vapor rinsing treatment of the p-type layer of the battery (4) with the absorbing layer is carried out at 2 mbar during 10 20 sec, and the p-type layer and the accretion by the microcrystalline enthalpy (10) This steam rinsing treatment was carried out at a vapor pressure of 1,200 seconds. The method is carried out by a steam of water vapor. The water pressure pressure layer between the two is 1.2 mbar -20-
TW100131603A 2010-09-03 2011-09-02 Method for thin film silicon photovoltaic cell production TW201216491A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US37987010P 2010-09-03 2010-09-03

Publications (1)

Publication Number Publication Date
TW201216491A true TW201216491A (en) 2012-04-16

Family

ID=44532877

Family Applications (1)

Application Number Title Priority Date Filing Date
TW100131603A TW201216491A (en) 2010-09-03 2011-09-02 Method for thin film silicon photovoltaic cell production

Country Status (3)

Country Link
CN (1) CN103262263A (en)
TW (1) TW201216491A (en)
WO (1) WO2012028684A2 (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004038774A2 (en) 2002-10-25 2004-05-06 Unaxis Balzers Ltd. Method for producing semi-conducting devices and devices obtained with this method
CN202217689U (en) * 2008-04-18 2012-05-09 欧瑞康太阳能股份公司(特吕巴赫) Photovoltaic device and photovoltaic converter panel including same
WO2010046180A2 (en) * 2008-10-22 2010-04-29 Applied Materials Inc. - A Corporation Of The State Of Delaware Semiconductor device and method of producing a semiconductor device

Also Published As

Publication number Publication date
WO2012028684A2 (en) 2012-03-08
CN103262263A (en) 2013-08-21
WO2012028684A3 (en) 2012-06-21

Similar Documents

Publication Publication Date Title
TWI438904B (en) Thin film solar cell and method of manufacturing same
CN101820007B (en) High-conversion rate silicon and thin film compound type multijunction PIN solar cell and manufacturing method thereof
CN101866963B (en) Silicon-based multijunction multi-laminated PIN thin film solar cell with high conversion rate and production method thereof
AU2015279725B2 (en) Passivation of light-receiving surfaces of solar cells with crystalline silicon
US20150136210A1 (en) Silicon-based solar cells with improved resistance to light-induced degradation
JP2021523580A (en) Semi-laminated flexible silicon-based thin-film solar cell and its manufacturing method
CN101567404A (en) Silicon-based thin-film solar cell structure with multi-junction structure and process thereof
US20100229912A1 (en) Photovoltaic device through lateral crystallization process and fabrication method thereof
CN102770966A (en) Thin film photoelectric conversion device and process for production thereof
TW201133881A (en) Thin film solar cell and manufacturing method thereof
CN101820006B (en) High-conversion rate silicon-based unijunction multi-laminate PIN thin-film solar cell and manufacturing method thereof
US20130298987A1 (en) Method for manufacturing a multilayer of a transparent conductive oxide
CN103563091A (en) Tandem solar cell with improved tunnel junction
CN101894871B (en) High-conversion rate silicon crystal and thin film compound type unijunction PIN (Positive Intrinsic-Negative) solar battery and manufacturing method thereof
WO2010022530A1 (en) Method for manufacturing transparent conductive oxide (tco) films; properties and applications of such films
CN102138220A (en) Method for depositing an amorphous silicon film for photovoltaic devices with reduced light- induced degradation for improved stabilized performance
TW201041165A (en) Solar battery and method for manufacturing the same
TW201001731A (en) Photovoltaic device and method of manufacturing a photovoltaic device
TW201216491A (en) Method for thin film silicon photovoltaic cell production
Lien et al. Effects of RF power and pressure on performance of HF-PECVD silicon thin-film solar cells
CN101499496A (en) Silicon thin film solar cell
TW201019483A (en) Improvement of electrical and optical properties of silicon solar cells
WO2013102576A1 (en) Intermediate reflection structure in thin film solar cells
TW200933908A (en) A silicon-based thin film solar-cell
KR20120054828A (en) Silicon solar cell having ultra high efficiency and preparation method thereof