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SnO和C60的电学性质对p-i-n结构半透明钙钛矿太阳能电池载流子传输特性的影响

Effects of the Electrical Properties of SnO and C60 on the Carrier Transport Characteristics of p-i-n-Structured Semitransparent Perovskite Solar Cells.

作者信息

Pham Hoang Minh, Naqvi Syed Dildar Haider, Tran Huyen, Tran Hung Van, Delda Jonabelle, Hong Sungjun, Jeong Inyoung, Gwak Jihye, Ahn SeJin

机构信息

Photovoltaics Research Department, Korea Institute of Energy Research, Daejeon 34129, Republic of Korea.

Department of Renewable Energy Engineering, University of Science and Technology, Daejeon 34113, Republic of Korea.

出版信息

Nanomaterials (Basel). 2023 Dec 6;13(24):3091. doi: 10.3390/nano13243091.

DOI:10.3390/nano13243091
PMID:38132989
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10745447/
Abstract

Recently, metal halide perovskite-based top cells have shown significant potential for use in inexpensive and high-performance tandem solar cells. In state-of-the-art p-i-n perovskite/Si tandem devices, atomic-layer-deposited SnO has been widely used as a buffer layer in the top cells because it enables conformal, pinhole-free, and highly transparent buffer layer formation. In this work, the effects of various electrical properties of SnO and C60 layers on the carrier transport characteristics and the performance of the final devices were investigated using a numerical simulation method, which was established based on real experimental data to increase the validity of the model. It was found that the band alignment at the SnO/C60 interface does, indeed, have a significant impact on the electron transport. In addition, as a general design rule, it was suggested that at first, the conduction band offset (CBO) between C60 and SnO should be chosen so as not to be too negative. However, even in a case in which this CBO condition is not met, we would still have the means to improve the electron transport characteristics by increasing the doping density of at least one of the two layers of C60 and/or SnO, which would enhance the built-in potential across the perovskite layer and the electron extraction at the C60/SnO interface.

摘要

最近,基于金属卤化物钙钛矿的顶电池在用于廉价且高性能的串联太阳能电池方面显示出巨大潜力。在最先进的p-i-n钙钛矿/硅串联器件中,原子层沉积的SnO已被广泛用作顶电池中的缓冲层,因为它能够形成保形、无针孔且高度透明的缓冲层。在这项工作中,使用一种基于实际实验数据建立的数值模拟方法,研究了SnO和C60层的各种电学性质对载流子传输特性和最终器件性能的影响,以提高模型的有效性。研究发现,SnO/C60界面处的能带排列确实对电子传输有重大影响。此外,作为一般设计规则,建议首先选择C60和SnO之间的导带偏移(CBO),使其不要过于负向。然而,即使在不满足此CBO条件的情况下,我们仍有办法通过提高C60和/或SnO两层中至少一层的掺杂密度来改善电子传输特性,这将增强钙钛矿层上的内建电势以及C60/SnO界面处的电子提取。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/6c1e953f1448/nanomaterials-13-03091-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/9cf1896c48e6/nanomaterials-13-03091-g001.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/0a7ae34dc996/nanomaterials-13-03091-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/2bba16d1b831/nanomaterials-13-03091-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/6c1e953f1448/nanomaterials-13-03091-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/9cf1896c48e6/nanomaterials-13-03091-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/5a498ebd498d/nanomaterials-13-03091-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/212ebd2c80da/nanomaterials-13-03091-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/1db45a015cf3/nanomaterials-13-03091-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/9d95dadb9300/nanomaterials-13-03091-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/606b580312f9/nanomaterials-13-03091-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/0a7ae34dc996/nanomaterials-13-03091-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/2bba16d1b831/nanomaterials-13-03091-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e86/10745447/6c1e953f1448/nanomaterials-13-03091-g009.jpg

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