用于柔性设备的无 ETL 双面过氧化物太阳能电池的性能优化:模拟研究

Numeshwar Kumar Sinha , Priyanka Roy , Dhriti Sundar Ghosh , Ayush Khare
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摘要

柔性过氧化物太阳能电池(PSCs)的广泛应用使其成为我们日常生活中大有可为的能量收集装置。无电子传输层(ETL)的 PSC 为利用能源提供了一种灵活的方法,同时增加了一种双面方法,可进一步提高器件性能。在我们的研究中,我们通过模拟选择合适的前透明电极(FTE)、空穴传输层(HTL)和后透明电极(RTE),优化了无 ETL 双面 PSCs。我们的研究发现,潜在的井状结构与 FTE/perovskite 界面上的小导带偏移 (CBO) 相关联,具有提高器件功率转换效率 (PCE) 的巨大潜力。HTL 价带的上移会促进重组,降低器件性能。RTE 的带隙和电子亲和力对 HTL/RTE 界面的能带排列有很大影响。NiO/Ag/NiO(NAN)三层 RTE 与 HTL 的能带排列更好,改善了电荷传输,从而提高了器件性能。此外,FTE/过氧化物和过氧化物/HTL 界面的界面缺陷层厚度也会对器件性能产生重大影响。在优化透辉石吸收层时,1.4 eV 的透辉石带隙显示出最高的器件性能。我们优化后的器件在正面和背面照明下的 PCE 都达到了 27%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Performance optimization of ETL-free bifacial perovskite solar cells for flexible devices: A simulation study

Performance optimization of ETL-free bifacial perovskite solar cells for flexible devices: A simulation study

The versatile applications of flexible perovskite solar cells (PSCs) have made them promising energy-harvesting devices in our daily lives. The electron transport layer (ETL)-free PSCs offer a flexible approach for harnessing energy while adding a bifacial approach that can further improve the device performance. In our study, we have optimized ETL-free bifacial PSCs via simulation by selecting the suitable front transparent electrode (FTE), hole transport layer (HTL), and rear transparent electrode (RTE). Our investigation reveals that a potential well-like structure, associated with a small conduction band offset (CBO) at the FTE/perovskite interface holds significant potential for enhancing the power conversion efficiency (PCE) of the device. The upward shift in the valance band of HTL promotes recombination and reduces the device performance. The bandgap and electron affinity of RTE highly influence the band alignment at HTL/RTE interface. The NiO/Ag/NiO (NAN) tri-layer RTE provides a better band alignment with HTL, and improves the charge transportation and, hence, the device performance. Moreover, the thickness of the interfacial defect layer at the FTE/perovskite and perovskite/HTL interfaces significantly impacts device performance. In optimizing the perovskite absorber layer, a perovskite bandgap of 1.4 eV shows maximum device performance. Our optimized device shows a remarkable PCE of >27% for both front and rear illumination.

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