TWI596785B - Solar cell structure and method for manufacturing the same - Google Patents

Solar cell structure and method for manufacturing the same Download PDF

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TWI596785B
TWI596785B TW105131556A TW105131556A TWI596785B TW I596785 B TWI596785 B TW I596785B TW 105131556 A TW105131556 A TW 105131556A TW 105131556 A TW105131556 A TW 105131556A TW I596785 B TWI596785 B TW I596785B
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solar cell
cell structure
titanium oxide
forming
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TW201714318A (en
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徐為哲
詹盛文
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財團法人工業技術研究院
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    • 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
    • H01L31/0248Semiconductor 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 characterised by their semiconductor bodies
    • H01L31/0352Semiconductor 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 characterised by their semiconductor bodies characterised by their shape or by the shapes, relative sizes or disposition of the semiconductor regions
    • H01L31/035272Semiconductor 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 characterised by their semiconductor bodies characterised by their shape or by the shapes, relative sizes or disposition of the semiconductor regions characterised by at least one potential jump barrier or surface barrier
    • 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
    • H01L31/02Details
    • H01L31/0224Electrodes
    • H01L31/022466Electrodes made of transparent conductive layers, e.g. TCO, ITO layers
    • H01L31/022475Electrodes made of transparent conductive layers, e.g. TCO, ITO layers composed of indium tin oxide [ITO]
    • 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
    • H01L31/02Details
    • H01L31/0224Electrodes
    • H01L31/022466Electrodes made of transparent conductive layers, e.g. TCO, ITO layers
    • H01L31/022483Electrodes made of transparent conductive layers, e.g. TCO, ITO layers composed of zinc oxide [ZnO]
    • 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
    • H01L31/1828Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof the active layers comprising only AIIBVI compounds, e.g. CdS, ZnS, CdTe
    • H01L31/1832Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof the active layers comprising only AIIBVI compounds, e.g. CdS, ZnS, CdTe comprising ternary compounds, e.g. Hg Cd Te
    • 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

Description

太陽能電池結構與其形成方法 Solar cell structure and forming method thereof

本發明係關於太陽能電池,更特別關於其結構及形成方法。 This invention relates to solar cells, and more particularly to their construction and method of formation.

近年來全球工業蓬勃發展,雖然利用傳統的能源供給方法成本較便宜,但卻潛在著輻射及環境汙染等問題。因此綠色替代能源成為各研究單位的研發重點,其中以太陽能電池最受矚目。傳統太陽電池主要以矽晶為主,但近年來各種薄膜太陽能電池蓬勃發展,但若考慮無毒、高效率以及高穩定度則以銅銦硒系列太陽能電池為首選。 In recent years, the global industry has flourished. Although the traditional energy supply method is cheaper, it has potential problems such as radiation and environmental pollution. Therefore, green alternative energy has become the focus of research and development of various research units, among which solar cells are the most eye-catching. Traditional solar cells are mainly dominated by twins. However, in recent years, various thin film solar cells have flourished. However, copper, indium and selenium series solar cells are preferred if nontoxic, high efficiency and high stability are considered.

銅銦鎵硒(CIGS)是一種黃銅礦結構的化合物,其晶體結構為正方結構,因為擁有高光學吸收係數、吸光波段範圍廣、化學性質穩定性高、以及直接能隙的優點,因此相當適合做為太陽能電池的材料。一般的CIGS電池於基板上依序為電極層、CIGS層、CdS層、i-ZnO層、AZO層、以及視情況形成的指狀電極。CdS層上的i-ZnO層可減緩緩衝層覆蓋不完全的問題,並有效抑制電池的漏電流。此外,i-ZnO層可降低濺鍍AZO層時,離子轟擊對CdS層的破壞。但i-ZnO層的厚度一般高達50nm至100nm,因此吸收部分入射光而降低太陽能電池的效 率。另一方面,i-ZnO層阻值大而不利電流蒐集。 Copper indium gallium selenide (CIGS) is a chalcopyrite structure compound with a crystal structure of a square structure. Because of its high optical absorption coefficient, wide range of absorption bands, high chemical stability, and direct energy gap, it is equivalent. Suitable as a material for solar cells. A general CIGS battery is sequentially an electrode layer, a CIGS layer, a CdS layer, an i-ZnO layer, an AZO layer, and a finger electrode formed as appropriate on the substrate. The i-ZnO layer on the CdS layer can alleviate the problem of incomplete buffer layer coverage and effectively suppress the leakage current of the battery. In addition, the i-ZnO layer can reduce the damage of the CdS layer by ion bombardment when the AZO layer is sputtered. However, the thickness of the i-ZnO layer is generally as high as 50 nm to 100 nm, so that part of the incident light is absorbed to reduce the efficiency of the solar cell. rate. On the other hand, the i-ZnO layer has a large resistance value and is not suitable for current collection.

綜上所述,目前需要新的CIGS電池結構以克服習知i-ZnO層所導致的問題。 In summary, new CIGS cell structures are currently needed to overcome the problems caused by conventional i-ZnO layers.

本發明一實施例提供之太陽能電池結構,包括:基板;金屬電極,位於基板上;吸收層,位於金屬電極上;緩衝層,位於吸收層上;氧化鈦層,位於緩衝層上,且氧化鈦層之厚度大於0且小於10nm;以及透明導電氧化物層,位於氧化鈦層上。 A solar cell structure according to an embodiment of the invention includes: a substrate; a metal electrode on the substrate; an absorption layer on the metal electrode; a buffer layer on the absorption layer; a titanium oxide layer on the buffer layer, and titanium oxide The layer has a thickness greater than 0 and less than 10 nm; and a transparent conductive oxide layer on the titanium oxide layer.

本發明一實施例提供之太陽能電池結構的形成方法,包括:形成金屬電極於基板上;形成吸收層於金屬電極上;形成緩衝層於吸收層上;形成氧化鈦層於緩衝層上,且氧化鈦層之厚度大於0且小於10nm;以及形成透明導電氧化物層於氧化鈦層上,其中形成氧化鈦層於緩衝層上之步驟為原子層沉積,該原子層沉積之溫度介於100℃至180℃之間,且原子層沉積之前驅物為四異丙氧基鈦。 A method for forming a solar cell structure according to an embodiment of the present invention includes: forming a metal electrode on a substrate; forming an absorption layer on the metal electrode; forming a buffer layer on the absorption layer; forming a titanium oxide layer on the buffer layer, and oxidizing The thickness of the titanium layer is greater than 0 and less than 10 nm; and the transparent conductive oxide layer is formed on the titanium oxide layer, wherein the step of forming the titanium oxide layer on the buffer layer is atomic layer deposition, and the temperature of the atomic layer deposition is between 100 ° C and Between 180 ° C, and the precursor before atomic layer deposition is titanium tetraisopropoxide.

10‧‧‧基板 10‧‧‧Substrate

11‧‧‧金屬電極 11‧‧‧Metal electrodes

13‧‧‧吸收層 13‧‧‧absorbing layer

15‧‧‧緩衝層 15‧‧‧buffer layer

17‧‧‧氧化鈦層 17‧‧‧Titanium oxide layer

19‧‧‧透明導電氧化物層 19‧‧‧Transparent conductive oxide layer

21‧‧‧指狀電極 21‧‧‧ finger electrodes

100‧‧‧太陽能電池 100‧‧‧ solar cells

第1圖係本發明一實施例中,太陽能電池的示意圖。 Fig. 1 is a schematic view showing a solar cell in an embodiment of the present invention.

第1圖係本發明一實施例中,太陽能電池100的示意圖。首先提供基板10如塑膠、不繡鋼、玻璃、石英、或其他常見基板材質。接著形成金屬電極11於基板10上,其形成方法可為濺鍍、物理氣相沉積、或噴塗法等。在本發明一實施例中, 金屬電極11可為鉻、鉬、銅、銀、金、鉑、其他金屬、或上述之合金。接著形成吸收層13於金屬電極11上。在本發明一實施例中,吸收層13可為銅銦鎵硒(CIGS)、銅銦鎵硒硫(CIGSS)、銅鎵硒(CGS)、銅鎵硒硫(CGSS)、或銅銦硒(CIS)。吸收層13的形成方法可為蒸鍍法、濺鍍法、電鍍法、或奈米粒子塗佈等方法,請參考Solar Energy,77(2004)page 749-756與Thin Solid Films,480-481(2005)page 99-109。 1 is a schematic view of a solar cell 100 in an embodiment of the present invention. First, a substrate 10 such as plastic, stainless steel, glass, quartz, or other common substrate materials is provided. Next, a metal electrode 11 is formed on the substrate 10, which may be formed by sputtering, physical vapor deposition, or spray coating. In an embodiment of the invention, The metal electrode 11 may be chromium, molybdenum, copper, silver, gold, platinum, other metals, or alloys thereof. Next, an absorbing layer 13 is formed on the metal electrode 11. In an embodiment of the invention, the absorbing layer 13 may be copper indium gallium selenide (CIGS), copper indium gallium selenide (CIGSS), copper gallium selenide (CGS), copper gallium selenide (CGSS), or copper indium selenide ( CIS). The method for forming the absorption layer 13 may be a vapor deposition method, a sputtering method, a plating method, or a method of coating a nano particle, and is referred to Solar Energy, 77 (2004) page 749-756 and Thin Solid Films, 480-481 ( 2005) page 99-109.

接著形成緩衝層15於吸收層13上。在本發明一實施例中,緩衝層15可為硫化鎘、硫化鋅、氧化錫鋅、氧化鋅、氧化鋅鎂或硫化銦。在本發明一實施例中,緩衝層15之厚度大於0且小於或等於30nm。若太陽能電池100不具有緩衝層15(即後續形成之TiO2層17直接接觸吸收層13),則需要一段時間(比如10分鐘至1小時)才會達到最高效率。若緩衝層15之厚度過大,除了使穿透光量下降外,也將因串聯電阻大幅提高而導致電池效率下降。上述緩衝層15之形成方法可參考Solar Energy,77(2004)page 749-756,使用的化學藥品為硫酸鎘(或硫酸銦)、硫脲、以及氨水,操作溫度約為50℃~75℃之間。 A buffer layer 15 is then formed on the absorber layer 13. In an embodiment of the invention, the buffer layer 15 may be cadmium sulfide, zinc sulfide, zinc tin oxide, zinc oxide, zinc magnesium oxide or indium sulfide. In an embodiment of the invention, the buffer layer 15 has a thickness greater than zero and less than or equal to 30 nm. If the solar cell 100 does not have the buffer layer 15 (i.e., the subsequently formed TiO 2 layer 17 is in direct contact with the absorbing layer 13), it takes a period of time (e.g., 10 minutes to 1 hour) to achieve the highest efficiency. If the thickness of the buffer layer 15 is too large, in addition to a decrease in the amount of transmitted light, the battery efficiency will be lowered due to a large increase in series resistance. The method for forming the buffer layer 15 can be referred to Solar Energy, 77 (2004) page 749-756, and the chemicals used are cadmium sulfate (or indium sulfate), thiourea, and ammonia water, and the operating temperature is about 50 ° C to 75 ° C. between.

接著以原子層沉積形成該氧化鈦層17於緩衝層15上,原子層沉積之溫度介於100℃至180℃之間,且原子層沉積之前驅物可為四異丙氧基鈦。若原子層沉積之溫度過高,則會損傷吸收層13。若原子層沉積之溫度過低,除了鍍膜速度大幅下降外,也無法去除前驅物中的碳,因此使薄膜品質大幅下降。在本發明一實施例中,氧化鈦層17為非晶相。值得注意的是,用於原子層沉積之前驅物不可含鹵素如TiCl4、TiBr4、或 類似物,以避免沉積過程中產生的鹵素腐蝕下方之緩衝層15(甚至是吸收層13)。在本發明一實施例中,氧化鈦層17之厚度大於0且小於10nm。若氧化鈦層17之厚度過厚,則會使穿透光量下降,進而降低電池效率。若氧化鈦層17不存在(即後續形成之透明導電氧化物層19直接接觸緩衝層15),則無法有效抑制電池的漏電流,亦無法避免濺鍍透明導電氧化物層19時離子轟擊對緩衝層15的破壞。另一方面,氧化鈦層17之厚度與吸收層13的組成相關。舉例來說,若吸收層13為銅銦鎵硒(CIGS),則氧化鈦層17之厚度大於0且小於10nm。 The titanium oxide layer 17 is then deposited on the buffer layer 15 by atomic layer deposition, the atomic layer deposition temperature is between 100 ° C and 180 ° C, and the precursor before the atomic layer deposition may be titanium tetraisopropoxide. If the temperature at which the atomic layer is deposited is too high, the absorption layer 13 is damaged. If the temperature at which the atomic layer is deposited is too low, in addition to a drastic decrease in the coating speed, the carbon in the precursor cannot be removed, so that the film quality is greatly degraded. In an embodiment of the invention, the titanium oxide layer 17 is an amorphous phase. It is worth noting that the precursor may not contain a halogen such as TiCl 4 , TiBr 4 , or the like prior to atomic layer deposition to avoid corrosion of the buffer layer 15 (or even the absorbing layer 13) underneath the halogen generated during deposition. In an embodiment of the invention, the thickness of the titanium oxide layer 17 is greater than 0 and less than 10 nm. If the thickness of the titanium oxide layer 17 is too thick, the amount of transmitted light is lowered, and the battery efficiency is further lowered. If the titanium oxide layer 17 is absent (ie, the subsequently formed transparent conductive oxide layer 19 directly contacts the buffer layer 15), the leakage current of the battery cannot be effectively suppressed, and the ion bombardment buffering when the transparent conductive oxide layer 19 is sputtered cannot be avoided. Destruction of layer 15. On the other hand, the thickness of the titanium oxide layer 17 is related to the composition of the absorption layer 13. For example, if the absorbing layer 13 is copper indium gallium selenide (CIGS), the thickness of the titanium oxide layer 17 is greater than 0 and less than 10 nm.

接著形成透明導電氧化物層19於氧化鈦層17上。在本發明一實施例中,透明導電氧化物層19可為銦錫氧化物(ITO)、銦鋅氧化物(IZO)、鋁鋅氧化物(AZO)、鎵鋅氧化物(GZO)、鋁鎵鋅氧化物(AGZO)、鎘錫氧化物、氧化鋅、二氧化鋯、或其他透明導電材料。透明導電氧化物層19的形成方法可為濺鍍法、蒸鍍法、原子層沉積法、熱裂解法、奈米粒子塗佈法、及其他相關製程。 A transparent conductive oxide layer 19 is then formed on the titanium oxide layer 17. In an embodiment of the invention, the transparent conductive oxide layer 19 may be indium tin oxide (ITO), indium zinc oxide (IZO), aluminum zinc oxide (AZO), gallium zinc oxide (GZO), aluminum gallium. Zinc oxide (AGZO), cadmium tin oxide, zinc oxide, zirconium dioxide, or other transparent conductive material. The transparent conductive oxide layer 19 can be formed by a sputtering method, an evaporation method, an atomic layer deposition method, a thermal cracking method, a nanoparticle coating method, and the like.

在本發明一實施例中,可視情況形成指狀電極21於透明導電氧化物層19上。指狀電極21的材質可為鎳鋁合金,其形成方法可為濺鍍、微影、蝕刻、及/或其他合適製程。在本發明一實施例中,當透明導電氧化物層19的表面積較小時,可省略指狀電極21。 In an embodiment of the invention, the finger electrodes 21 are formed on the transparent conductive oxide layer 19 as appropriate. The finger electrode 21 may be made of a nickel-aluminum alloy, and may be formed by sputtering, lithography, etching, and/or other suitable processes. In an embodiment of the invention, when the surface area of the transparent conductive oxide layer 19 is small, the finger electrodes 21 may be omitted.

與習知夾設於緩衝層與透明導電氧化物層之間的i-ZnO層相較,上述氧化鈦層17具有較小的電阻以及較高的入光量,可使太陽能電池具有較佳之光電轉換效率。 Compared with the i-ZnO layer which is conventionally sandwiched between the buffer layer and the transparent conductive oxide layer, the above titanium oxide layer 17 has a small electrical resistance and a high light incident amount, so that the solar cell can have better photoelectric conversion. effectiveness.

為了讓本發明之上述和其他目的、特徵、和優點能更明顯易懂,下文特舉數實施例配合所附圖示,作詳細說明如下: The above and other objects, features, and advantages of the present invention will become more apparent and understood.

實施例 Example

實施例1(氧化鈦層夾設於緩衝層與透明導電氧化物層之間) Example 1 (the titanium oxide layer is interposed between the buffer layer and the transparent conductive oxide layer)

首先於不鏽鋼基板上透過濺鍍製程分別鍍製1000nm的Cr以及Mo作為金屬電極。之後以塗佈方式將CuInGa奈米粒子氧化前驅物塗佈於Mo膜之上,再透過還原、硒硫化製程以製備CIGSeS吸收層(約3000nm)。接著使用5wt% KCN水溶液清潔CIGSeS吸收層以去除銅硒化合物,即形成吸收層。接著以化學浴法鍍製50nm厚之CdS薄膜於吸收層上以作為緩衝層,其中化學浴法的溫度控制於65℃。接著以原子層沉積法製備3nm厚之氧化鈦層於緩衝層上,此製程溫度控於120℃,且前驅物為四異丙氧基鈦。之後再鍍製300nm之AZO層於氧化鈦層上作為透明導電氧化物層,最後再於透明導電氧化物層上鍍製Ni-Al指狀電極,以完成太陽能電池結構。 First, 1000 nm of Cr and Mo were respectively plated on the stainless steel substrate through a sputtering process as metal electrodes. Then, a CuInGa nanoparticle oxidation precursor is coated on the Mo film by a coating method, and then passed through a reduction and selenization process to prepare a CIGSeS absorption layer (about 3000 nm). The CIGSeS absorber layer was then cleaned using a 5 wt% KCN aqueous solution to remove the copper selenium compound, i.e., to form an absorber layer. Next, a 50 nm thick CdS film was plated on the absorption layer by a chemical bath method to serve as a buffer layer, wherein the temperature of the chemical bath method was controlled at 65 °C. Then, a 3 nm thick titanium oxide layer was prepared on the buffer layer by atomic layer deposition, the process temperature was controlled at 120 ° C, and the precursor was titanium tetraisopropoxide. Then, a 300 nm AZO layer was plated on the titanium oxide layer as a transparent conductive oxide layer, and finally a Ni-Al finger electrode was plated on the transparent conductive oxide layer to complete the solar cell structure.

實施例2-1及2-2 Examples 2-1 and 2-2

與實施例1類似,差別在於氧化鈦層之厚度增加至5nm。 Similar to Example 1, the difference was that the thickness of the titanium oxide layer was increased to 5 nm.

實施例3 Example 3

與實施例1類似,差別在於氧化鈦層之厚度增加至7nm。 Similar to Example 1, the difference was that the thickness of the titanium oxide layer was increased to 7 nm.

實施例4 Example 4

與實施例1類似,差別在於氧化鈦層之厚度增加至9nm。 Similar to Example 1, the difference was that the thickness of the titanium oxide layer was increased to 9 nm.

實施例5 Example 5

與實施例1類似,差別在於氧化鈦層之厚度增加至10nm。 Similar to Example 1, the difference was that the thickness of the titanium oxide layer was increased to 10 nm.

實施例6 Example 6

與實施例1類似,差別在於氧化鈦層之厚度增加至15nm。 Similar to Example 1, the difference was that the thickness of the titanium oxide layer was increased to 15 nm.

實施例7 Example 7

與實施例1類似,差別在於氧化鈦層之厚度增加至30nm。 Similar to Example 1, the difference was that the thickness of the titanium oxide layer was increased to 30 nm.

比較例1至7(i-ZnO層夾設於緩衝層與透明導電氧化物層之間) Comparative Examples 1 to 7 (i-ZnO layer is interposed between the buffer layer and the transparent conductive oxide layer)

首先於不鏽鋼基板上透過濺鍍製程分別鍍製1000nm的Cr以及Mo作為金屬電極。之後以塗佈方式將CuInGa奈米粒子氧化前驅物塗佈於Mo膜之上,再透過還原、硒硫化製程以製備CIGSeS吸收層(約3000nm)。接著使用5wt% KCN水溶液清潔CIGSeS吸收層以去除銅硒化合物,即形成吸收層。接著以化學浴法鍍製50nm厚之CdS薄膜於吸收層上以作為緩衝層,其中化學浴法的溫度控制於65℃。接著以濺鍍製程製備50nm厚之i-ZnO層於緩衝層上,再鍍製300nm之AZO層於i-ZnO層上作為透明導電氧化物層,最後再於透明導電氧化物層上鍍製Ni-Al指狀電極,以完成比較例之太陽能電池結構。 First, 1000 nm of Cr and Mo were respectively plated on the stainless steel substrate through a sputtering process as metal electrodes. Then, a CuInGa nanoparticle oxidation precursor is coated on the Mo film by a coating method, and then passed through a reduction and selenization process to prepare a CIGSeS absorption layer (about 3000 nm). The CIGSeS absorber layer was then cleaned using a 5 wt% KCN aqueous solution to remove the copper selenium compound, i.e., to form an absorber layer. Next, a 50 nm thick CdS film was plated on the absorption layer by a chemical bath method to serve as a buffer layer, wherein the temperature of the chemical bath method was controlled at 65 °C. Then, a 50 nm thick i-ZnO layer is prepared on the buffer layer by a sputtering process, and then a 300 nm AZO layer is plated on the i-ZnO layer as a transparent conductive oxide layer, and finally a Ni is plated on the transparent conductive oxide layer. - Al finger electrode to complete the solar cell structure of the comparative example.

上述比較例與實施例在形成i-ZnO層/氧化鈦層之前屬於相同結構。在實驗上,可在形成緩衝層後將太陽能電池的半成品分成兩組面積相同的半成品,再分別形成i-ZnO/AZO/Ni-Al指狀電極(比較例1至7)與氧化鈦層/AZO/Ni-Al指狀電極(實施例1至7)。 The above comparative examples and the examples belong to the same structure before the formation of the i-ZnO layer/titanium oxide layer. Experimentally, the semi-finished product of the solar cell can be divided into two sets of semi-finished products having the same area after forming the buffer layer, and then the i-ZnO/AZO/Ni-Al finger electrodes (Comparative Examples 1 to 7) and the titanium oxide layer are respectively formed. AZO/Ni-Al finger electrodes (Examples 1 to 7).

如第1至8表所示,可比較不同的氧化鈦層厚度對電池電性的影響。隨著厚度增加(5nm至30nm),太陽能電池之 Voc下降(0.564V to 0.541V),即過長的原子層沉積(ALD)時間造成Cd離子的過度擴散而降低電池的Voc。此外,隨著氧化鈦厚度增加,實施例之電池的Jsc亦些微下降。隨著氧化鈦層厚度增加,太陽能電池的F.F.明顯下降,主要原因為Rsh下降以及Rs上升所致。綜上所述,當氧化鈦層厚度增加,太陽能電池的效率明顯下降(從12.96%(5nm)降至11.36%(30nm))。當氧化鈦層厚度自5nm(如實施例2-1,2-2)減少至3nm(如實施例1),實施例1之效率略低於實施例2-1及2-2之效率。 As shown in Tables 1 to 8, the effect of different thicknesses of the titanium oxide layer on the electrical properties of the battery can be compared. As the thickness increases (5 nm to 30 nm), the V oc of the solar cell decreases (0.564 V to 0.541 V), that is, excessively long atomic layer deposition (ALD) time causes excessive diffusion of Cd ions to lower the V oc of the battery. Further, as the thickness of the titanium oxide was increased, the J sc of the battery of the example was slightly lowered. As the thickness of the titanium oxide layer increases, the FF of the solar cell decreases significantly, mainly due to a decrease in R sh and an increase in R s . In summary, when the thickness of the titanium oxide layer is increased, the efficiency of the solar cell is significantly reduced (from 12.96% (5 nm) to 11.36% (30 nm)). When the thickness of the titanium oxide layer was reduced from 5 nm (as in Examples 2-1, 2-2) to 3 nm (as in Example 1), the efficiency of Example 1 was slightly lower than that of Examples 2-1 and 2-2.

如第4表所示,分別含有比較例3與實施例3中兩種不同結構之太陽能電池。由電性量測結果顯示,兩種結構之電池開路電壓(Voc)並無明顯變化。若比較電池之短路電流(Jsc),則實施例之太陽能電池比比較例之太陽能電池高約0.62mA/cm2(2.0%),推知應為氧化鈦薄膜具有較高光穿透度。若比較兩結構之填充因子(FF)則無明顯差別,即兩者之串聯電阻(Rs)與並聯電阻(Rsh)並無明顯差別。若比較兩者之電池效率,由第4表可知實施例之電池效率比比較例之電池效率高約0.25%,其效率提高原因主要為短路電流提升所致。 As shown in the fourth table, solar cells of two different structures in Comparative Example 3 and Example 3 were respectively contained. The electrical measurement results showed that the open circuit voltage (V oc ) of the two structures did not change significantly. When the short-circuit current (J sc ) of the battery was compared, the solar cell of the example was about 0.62 mA/cm 2 (2.0%) higher than that of the solar cell of the comparative example, and it was inferred that the titanium oxide film had a high light transmittance. If the fill factor (FF) of the two structures is compared, there is no significant difference, that is, the series resistance (R s ) of the two is not significantly different from the parallel resistance (R sh ). Comparing the battery efficiencies of the two, it can be seen from Table 4 that the battery efficiency of the embodiment is about 0.25% higher than that of the comparative example, and the increase in efficiency is mainly due to the increase in short-circuit current.

值得注意的是,太陽能電池的效率比較最好考慮相同電池上的比較例與實施例,以避免實驗誤差。舉例來說,第1表中實施例1比比較例1增加的效率應為(12.85-12.66)/12.66=+1.5%,第2表中實施例2-1比比較例2-1增加的效率應為(12.96-12.68)/12.68=+2.2%,第3表中實施例2-2比比較例2-2增加的效率應為(12.62-12.26)/12.26=+2.9%,第4表中實施例3比比較例3增加的效率應為 (12.78-12.53)/12.53=+2.0%,第5表中實施例4比比較例增加的效率應為(12.86-12.65)/12.65=+1.6%,第6表中實施例5比比較例增加的效率應為(12.72-12.56)/12.56=+1.2%,第7表中實施例6比比較例增加的效率應為(12.12-12.65)/12.65=-4.2%,而第8表中實施例7比比較例增加的效率應為(11.36-12.51)/12.51=-9.2%。綜上所述,氧化鈦層的厚度小於10nm時,比氧化鈦層的厚度大於或等於10nm時更能增加太陽能電池的效率(+1.5%)。 It is worth noting that the efficiency of solar cells is better considering the comparative examples and examples on the same battery to avoid experimental errors. For example, the efficiency of Example 1 in Table 1 is higher than that of Comparative Example 1 (12.85-12.66) / 12.66 = +1.5%, and the efficiency of Example 2-1 in Table 2 is higher than that of Comparative Example 2-1. Should be (12.96-12.68) / 12.68 = +2.2%, the efficiency of Example 2-2 in Table 3 is higher than that of Comparative Example 2-2 (12.62-12.26) / 12.26 = +2.9%, in Table 4 The efficiency of Example 3 over Comparative Example 3 should be (12.78-12.53) / 12.53 = +2.0%, and the efficiency of Example 4 in Table 5 should be (12.86-12.65) / 12.65 = +1.6%. The efficiency of Example 5 in Table 6 is higher than (1.72-12.56) / 12.56 = +1.2%, and the efficiency of Example 6 in Table 7 is higher than (12.12-12.65) / 12.65. =-4.2%, and the efficiency of Example 7 in Table 8 over the comparative example should be (11.36-12.51) / 12.51 = -9.2%. In summary, when the thickness of the titanium oxide layer is less than 10 nm, the efficiency of the solar cell can be increased more than when the thickness of the titanium oxide layer is greater than or equal to 10 nm ( +1.5%).

實施例8 Example 8

實施例8與實施例4類似,差別在於減少CdS之厚度至10nm。對應實施例8之電池製備方法與實施例4類似,差別在於此實施例之電池不具有比較例之太陽能電池結構。 Example 8 is similar to Example 4 except that the thickness of CdS is reduced to 10 nm. The battery preparation method corresponding to Example 8 was similar to that of Example 4 except that the battery of this example did not have the solar cell structure of the comparative example.

實施例9 Example 9

實施例9與實施例4類似,差別在於減少CdS之厚度至30nm。對應實施例9之電池製備方法與實施例4類似,差別在於此實施例之電池不具有比較例之太陽能電池結構。 Example 9 is similar to Example 4 except that the thickness of CdS is reduced to 30 nm. The battery preparation method corresponding to Example 9 was similar to that of Example 4 except that the battery of this example did not have the solar cell structure of the comparative example.

如第9表所示,厚度小於10nm之TiO2層可進一步減少CdS緩衝層的厚度(比如30nm,10nm)以改善電池效率。 As shown in the table 9, the TiO 2 layer having a thickness of less than 10 nm can further reduce the thickness of the CdS buffer layer (for example, 30 nm, 10 nm) to improve battery efficiency.

雖然本發明已以數個實施例揭露如上,然其並非用以限定本發明,任何所屬技術領域中具有通常知識者,在不脫離本發明之精神和範圍內,當可作些許之更動與潤飾,因此本發明之保護範圍當視後附之申請專利範圍所界定者為準。 The present invention has been disclosed in several embodiments, and is not intended to limit the scope of the present invention, and may be modified and modified without departing from the spirit and scope of the invention. Therefore, the scope of the invention is defined by the scope of the appended claims.

10‧‧‧基板 10‧‧‧Substrate

11‧‧‧金屬電極 11‧‧‧Metal electrodes

13‧‧‧吸收層 13‧‧‧absorbing layer

15‧‧‧緩衝層 15‧‧‧buffer layer

17‧‧‧氧化鈦層 17‧‧‧Titanium oxide layer

19‧‧‧透明導電氧化物層 19‧‧‧Transparent conductive oxide layer

21‧‧‧指狀電極 21‧‧‧ finger electrodes

100‧‧‧太陽能電池 100‧‧‧ solar cells

Claims (12)

一種太陽能電池結構,包括:一基板;一金屬電極,位於該基板上;一吸收層,位於該金屬電極上;一緩衝層,位於該吸收層上;氧化鈦層,位於該緩衝層上,且該氧化鈦層之厚度大於0且小於10nm;以及一透明導電氧化物層,位於該氧化鈦層上,其中該氧化鈦層為非晶相。 A solar cell structure comprising: a substrate; a metal electrode on the substrate; an absorbing layer on the metal electrode; a buffer layer on the absorbing layer; and a titanium oxide layer on the buffer layer, and The titanium oxide layer has a thickness greater than 0 and less than 10 nm; and a transparent conductive oxide layer is disposed on the titanium oxide layer, wherein the titanium oxide layer is an amorphous phase. 如申請專利範圍第1項所述之太陽能電池結構,其中該緩衝層之厚度大於0且小於或等於30nm。 The solar cell structure of claim 1, wherein the buffer layer has a thickness greater than 0 and less than or equal to 30 nm. 如申請專利範圍第1項所述之太陽能電池結構,其中該金屬電極包括鉻、鉬、銅、銀、金、鉑、或上述之合金。 The solar cell structure of claim 1, wherein the metal electrode comprises chromium, molybdenum, copper, silver, gold, platinum, or an alloy thereof. 如申請專利範圍第1項所述之太陽能電池結構,其中該吸收層包括銅銦鎵硒、銅銦鎵硒硫、銅鎵硒、銅鎵硒硫、或銅銦硒。 The solar cell structure of claim 1, wherein the absorbing layer comprises copper indium gallium selenide, copper indium gallium selenide, copper gallium selenide, copper gallium selenide, or copper indium selenide. 如申請專利範圍第4項所述之太陽能電池結構,其中該吸收層係銅銦鎵硒。 The solar cell structure of claim 4, wherein the absorbing layer is copper indium gallium selenide. 如申請專利範圍第1項所述之太陽能電池結構,其中該緩衝層包括硫化鎘、硫化鋅、氧化錫鋅、氧化鋅、氧化鋅鎂、或硫化銦。 The solar cell structure of claim 1, wherein the buffer layer comprises cadmium sulfide, zinc sulfide, zinc tin oxide, zinc oxide, zinc magnesium oxide, or indium sulfide. 如申請專利範圍第1項所述之太陽能電池結構,其中該透明導電氧化物層包括銦錫氧化物、銦鋅氧化物、鋁鋅氧化 物、鎵鋅氧化物、鋁鎵鋅氧化物、鎘錫氧化物、氧化鋅、或二氧化鋯。 The solar cell structure of claim 1, wherein the transparent conductive oxide layer comprises indium tin oxide, indium zinc oxide, aluminum zinc oxide , gallium zinc oxide, aluminum gallium zinc oxide, cadmium tin oxide, zinc oxide, or zirconium dioxide. 一種太陽能電池結構的形成方法,包括:形成一金屬電極於一基板上;形成一吸收層於該金屬電極上;形成一緩衝層於該吸收層上;形成氧化鈦層於該緩衝層上,且該氧化鈦層之厚度大於0且小於10nm;以及形成一透明導電氧化物層於該氧化鈦層上,其中形成該氧化鈦層於該緩衝層上之步驟為原子層沉積,該原子層沉積之溫度介於100℃至180℃之間,且該原子層沉積之前驅物為四異丙氧基鈦,其中該氧化鈦層為非晶相。 A method for forming a solar cell structure, comprising: forming a metal electrode on a substrate; forming an absorbing layer on the metal electrode; forming a buffer layer on the absorbing layer; forming a titanium oxide layer on the buffer layer, and The thickness of the titanium oxide layer is greater than 0 and less than 10 nm; and a transparent conductive oxide layer is formed on the titanium oxide layer, wherein the step of forming the titanium oxide layer on the buffer layer is atomic layer deposition, and the atomic layer is deposited The temperature is between 100 ° C and 180 ° C, and the precursor before the atomic layer deposition is titanium tetraisopropoxide, wherein the titanium oxide layer is an amorphous phase. 如申請專利範圍第8項所述之太陽能電池結構的形成方法,其中該緩衝層之厚度大於0且小於或等於30nm。 The method for forming a solar cell structure according to claim 8, wherein the buffer layer has a thickness greater than 0 and less than or equal to 30 nm. 如申請專利範圍第8項所述之太陽能電池結構的形成方法,其中該吸收層包括銅銦鎵硒、銅銦鎵硒硫、銅鎵硒、銅鎵硒硫、或銅銦硒。 The method for forming a solar cell structure according to claim 8, wherein the absorbing layer comprises copper indium gallium selenide, copper indium gallium selenide, copper gallium selenide, copper gallium selenide, or copper indium selenide. 如申請專利範圍第10項所述之太陽能電池結構的形成方法,其中該吸收層係銅銦鎵硒。 The method for forming a solar cell structure according to claim 10, wherein the absorbing layer is copper indium gallium selenide. 如申請專利範圍第8項所述之太陽能電池結構的形成方法,其中該緩衝層包括硫化鎘、硫化鋅、氧化錫鋅、氧化鋅、氧化鋅鎂或硫化銦。 The method for forming a solar cell structure according to claim 8, wherein the buffer layer comprises cadmium sulfide, zinc sulfide, zinc tin oxide, zinc oxide, zinc magnesium oxide or indium sulfide.
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