Thomas Paul Weiss, Mohit Sood, Aline Vanderhaegen, Susanne Siebentritt
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From photoluminescence spectroscopy, it is found that no additional non-radiative losses are introduced to the absorber when adding Te. However, \n<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>V</mi>\n <mi>OC</mi>\n </msub>\n </mrow>\n <annotation>$$ {V}_{OC} $$</annotation>\n </semantics></math> losses occur in the final solar cell due to non-optimized interfaces. Nevertheless, a device with 9% power conversion efficiency is demonstrated with a bandgap of 0.97 eV and \n<span></span><math>\n <semantics>\n <mrow>\n <mi>x</mi>\n <mo>=</mo>\n <mn>0.07</mn>\n </mrow>\n <annotation>$$ x&amp;#x0003D;0.07 $$</annotation>\n </semantics></math>, the highest efficiency so far for chalcopyrites with band gap <1 eV. Interface recombination is identified as a major recombination channel for larger Te contents. Thus, further efficiency improvements can be expected with improved absorber/buffer interfaces.</p>\n </div>","PeriodicalId":223,"journal":{"name":"Progress in Photovoltaics","volume":"33 2","pages":"253-264"},"PeriodicalIF":8.0000,"publicationDate":"2024-10-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"CuIn (Se,Te)2 Absorbers With Bandgaps <1 eV for Bottom Cells in Tandem Applications\",\"authors\":\"Thomas Paul Weiss, Mohit Sood, Aline Vanderhaegen, Susanne Siebentritt\",\"doi\":\"10.1002/pip.3851\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div>\\n \\n <p>Thin-film solar cells reach high efficiencies and have a low carbon footprint in production. Tandem solar cells have the potential to significantly increase the efficiency of this technology, where the bottom-cell is generally composed of a Cu(In,Ga)Se<sub>2</sub> absorber layer with bandgaps around 1 eV or higher. Here, we investigate CuIn(Se<sub>1 − x</sub>Te<sub>x</sub>)<sub>2</sub> absorber layers and solar cells with bandgaps below 1 eV, which will bring the benefit of an additional degree of freedom for designing current-matched two-terminal tandem devices. We report that CuIn(Se<sub>1 − x</sub>Te<sub>x</sub>)<sub>2</sub> thin films can be grown single phase by co-evaporation and that the bandgap can be reduced to the optimum range (0.92–0.95 eV) for a bottom cell. From photoluminescence spectroscopy, it is found that no additional non-radiative losses are introduced to the absorber when adding Te. However, \\n<span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>V</mi>\\n <mi>OC</mi>\\n </msub>\\n </mrow>\\n <annotation>$$ {V}_{OC} $$</annotation>\\n </semantics></math> losses occur in the final solar cell due to non-optimized interfaces. 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引用次数: 0
摘要
薄膜太阳能电池在生产过程中效率高,碳足迹低。串联太阳能电池具有显著提高该技术效率的潜力,其中底部电池通常由Cu(In,Ga)Se2吸收层组成,带隙约为1 eV或更高。在这里,我们研究了CuIn(Se1−xTex)2吸收层和带隙低于1ev的太阳能电池,这将为设计电流匹配的双端串联器件带来额外的自由度。我们报道了CuIn(Se1−xTex)2薄膜可以通过共蒸发单相生长,并且带隙可以减小到底部电池的最佳范围(0.92-0.95 eV)。从光致发光光谱分析中发现,当加入Te时,吸收剂没有引入额外的非辐射损失。然而,由于未优化界面,最终太阳能电池中会出现V OC $$ {V}_{OC} $$损失。然而,一个带有9% power conversion efficiency is demonstrated with a bandgap of 0.97 eV and x = 0.07 $$ x&#x0003D;0.07 $$ , the highest efficiency so far for chalcopyrites with band gap <1 eV. Interface recombination is identified as a major recombination channel for larger Te contents. Thus, further efficiency improvements can be expected with improved absorber/buffer interfaces.
CuIn (Se,Te)2 Absorbers With Bandgaps <1 eV for Bottom Cells in Tandem Applications
Thin-film solar cells reach high efficiencies and have a low carbon footprint in production. Tandem solar cells have the potential to significantly increase the efficiency of this technology, where the bottom-cell is generally composed of a Cu(In,Ga)Se2 absorber layer with bandgaps around 1 eV or higher. Here, we investigate CuIn(Se1 − xTex)2 absorber layers and solar cells with bandgaps below 1 eV, which will bring the benefit of an additional degree of freedom for designing current-matched two-terminal tandem devices. We report that CuIn(Se1 − xTex)2 thin films can be grown single phase by co-evaporation and that the bandgap can be reduced to the optimum range (0.92–0.95 eV) for a bottom cell. From photoluminescence spectroscopy, it is found that no additional non-radiative losses are introduced to the absorber when adding Te. However,
losses occur in the final solar cell due to non-optimized interfaces. Nevertheless, a device with 9% power conversion efficiency is demonstrated with a bandgap of 0.97 eV and
, the highest efficiency so far for chalcopyrites with band gap <1 eV. Interface recombination is identified as a major recombination channel for larger Te contents. Thus, further efficiency improvements can be expected with improved absorber/buffer interfaces.
期刊介绍:
Progress in Photovoltaics offers a prestigious forum for reporting advances in this rapidly developing technology, aiming to reach all interested professionals, researchers and energy policy-makers.
The key criterion is that all papers submitted should report substantial “progress” in photovoltaics.
Papers are encouraged that report substantial “progress” such as gains in independently certified solar cell efficiency, eligible for a new entry in the journal''s widely referenced Solar Cell Efficiency Tables.
Examples of papers that will not be considered for publication are those that report development in materials without relation to data on cell performance, routine analysis, characterisation or modelling of cells or processing sequences, routine reports of system performance, improvements in electronic hardware design, or country programs, although invited papers may occasionally be solicited in these areas to capture accumulated “progress”.