Terry Chien-Jen Yang, Taeheon Kang, Melissa Fitzsimmons, Guadalupe Vega, Yang Lu, Leo Rosado, Alberto Jiménez-Solano, Linfeng Pan, Szymon J Zelewski, Jordi Ferrer Orri, Yu-Hsien Chiang, Dengyang Guo, Zher Ying Ooi, Yutong Han, Weidong Xu, Bart Roose, Caterina Ducati, Sol Carretero Palacios, Miguel Anaya, Samuel D Stranks
{"title":"Incorporating thermal co-evaporation in current-matched all-perovskite triple-junction solar cells.","authors":"Terry Chien-Jen Yang, Taeheon Kang, Melissa Fitzsimmons, Guadalupe Vega, Yang Lu, Leo Rosado, Alberto Jiménez-Solano, Linfeng Pan, Szymon J Zelewski, Jordi Ferrer Orri, Yu-Hsien Chiang, Dengyang Guo, Zher Ying Ooi, Yutong Han, Weidong Xu, Bart Roose, Caterina Ducati, Sol Carretero Palacios, Miguel Anaya, Samuel D Stranks","doi":"10.1039/d4el00012a","DOIUrl":null,"url":null,"abstract":"<p><p>Thermal co-evaporation of halide perovskites is a solution-free, conformal, scalable, and controllable deposition technique with great potential for commercial applications, particularly in multi-junction solar cells. Monolithic triple-junction perovskite solar cells have garnered significant attention because they can achieve very high efficiencies. Nevertheless, challenges arise in fabricating these devices, as they require multiple layers and precise current matching across complex absorber stacks. Here we demonstrate a current-matched monolithic all-perovskite p-i-n triple-junction solar cell enabled by controlled thermal co-evaporation of various absorber layers in the stack. The top and middle subcells were fabricated by developing optimized thermally co-evaporated Cs<sub>0.3</sub>FA<sub>0.7</sub>Pb(I<sub>0.56</sub>Br<sub>0.44</sub>)<sub>3</sub> (1.80 eV bandgap) and FAPbI<sub>3</sub> (1.53 eV) perovskites, respectively, while the bottom subcell employed a solution-processed Cs<sub>0.25</sub>FA<sub>0.75</sub>Pb<sub>0.5</sub>Sn<sub>0.5</sub>I<sub>3</sub> (1.25 eV) perovskite. By optimising absorber thicknesses and compositions through optical modelling, we achieve excellent current matching between the top (9.6 mA cm<sup>-2</sup>), middle (9.3 mA cm<sup>-2</sup>), and bottom subcells (9.0 mA cm<sup>-2</sup>), achieving an overall efficiency of 15.8%. Optical modelling simulations suggest that current matching and efficiency up to 11.4 mA cm<sup>-2</sup> and 37.6% respectively could be attainable using the latest interlayer materials. This work highlights the potential of scalable vapour-based deposition techniques for advancing multi-junction perovskite-based solar cells, paving the way for future developments in this field.</p>","PeriodicalId":520395,"journal":{"name":"EES solar","volume":" ","pages":"41-55"},"PeriodicalIF":0.0000,"publicationDate":"2025-01-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11755821/pdf/","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"EES solar","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1039/d4el00012a","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/2/24 0:00:00","PubModel":"eCollection","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Thermal co-evaporation of halide perovskites is a solution-free, conformal, scalable, and controllable deposition technique with great potential for commercial applications, particularly in multi-junction solar cells. Monolithic triple-junction perovskite solar cells have garnered significant attention because they can achieve very high efficiencies. Nevertheless, challenges arise in fabricating these devices, as they require multiple layers and precise current matching across complex absorber stacks. Here we demonstrate a current-matched monolithic all-perovskite p-i-n triple-junction solar cell enabled by controlled thermal co-evaporation of various absorber layers in the stack. The top and middle subcells were fabricated by developing optimized thermally co-evaporated Cs0.3FA0.7Pb(I0.56Br0.44)3 (1.80 eV bandgap) and FAPbI3 (1.53 eV) perovskites, respectively, while the bottom subcell employed a solution-processed Cs0.25FA0.75Pb0.5Sn0.5I3 (1.25 eV) perovskite. By optimising absorber thicknesses and compositions through optical modelling, we achieve excellent current matching between the top (9.6 mA cm-2), middle (9.3 mA cm-2), and bottom subcells (9.0 mA cm-2), achieving an overall efficiency of 15.8%. Optical modelling simulations suggest that current matching and efficiency up to 11.4 mA cm-2 and 37.6% respectively could be attainable using the latest interlayer materials. This work highlights the potential of scalable vapour-based deposition techniques for advancing multi-junction perovskite-based solar cells, paving the way for future developments in this field.
卤化物钙钛矿的热共蒸发是一种无溶液、保形、可扩展和可控的沉积技术,具有巨大的商业应用潜力,特别是在多结太阳能电池中。单片三结钙钛矿太阳能电池已经引起了人们的极大关注,因为它们可以实现非常高的效率。然而,在制造这些器件的过程中出现了挑战,因为它们需要多层和复杂的吸收层之间的精确电流匹配。在这里,我们展示了一种电流匹配的单片全钙钛矿p-i-n三结太阳能电池,该电池通过控制堆叠中各种吸收层的热共蒸发而实现。顶部和中间亚电池分别采用优化的热共蒸发Cs0.3FA0.7Pb(I0.56Br0.44)3 (1.80 eV带隙)和FAPbI3 (1.53 eV)钙钛矿制备,底部亚电池采用溶液处理Cs0.25FA0.75Pb0.5Sn0.5I3 (1.25 eV)钙钛矿制备。通过光学建模优化吸收剂厚度和成分,我们实现了顶部(9.6 mA cm-2),中间(9.3 mA cm-2)和底部亚电池(9.0 mA cm-2)之间的良好电流匹配,实现了15.8%的总效率。光学模型模拟表明,使用最新的层间材料可以实现高达11.4 mA cm-2的电流匹配和37.6%的效率。这项工作强调了可扩展气相沉积技术在推进多结钙钛矿基太阳能电池方面的潜力,为该领域的未来发展铺平了道路。