From unstable CsSnI3 to air-stable Cs2SnI6: A lead-free perovskite solar cell light absorber with bandgap of 1.48 eV and high absorption coefficient

被引:447
作者
Qiu, Xiaofeng [1 ]
Cao, Bingqiang [1 ]
Yuan, Shuai [1 ]
Chen, Xiangfeng [1 ]
Qiu, Zhiwen [1 ]
Jiang, Yanan [1 ]
Ye, Qian [2 ]
Wang, Hongqiang [2 ]
Zeng, Haibo [3 ]
Liu, Jian [4 ]
Kanatzidis, Mercouri G. [4 ]
机构
[1] Univ Jinan, Sch Mat Sci & Engn, Mat Res Ctr Energy & Photoelectrochem Convers, Jinan 250022, Peoples R China
[2] Northwestern Polytech Univ, Sch Mat Sci & Engn, Ctr Nano Energy Mat, Xian 710072, Peoples R China
[3] Nanjing Univ Sci & Technol, Sch Mat Sci & Engn, Inst Optoelect & Nanomat, Nanjing 210094, Jiangsu, Peoples R China
[4] Northwestern Univ, Dept Chem, Evanston, IL 60208 USA
关键词
Perovskite absorber; Air-stable; Lead-free; Cs2SnI6; Solar cell; EFFICIENCY; TIN; DEPOSITION;
D O I
10.1016/j.solmat.2016.09.022
中图分类号
TE [石油、天然气工业]; TK [能源与动力工程];
学科分类号
0807 ; 0820 ;
摘要
All-inorganic and lead-free cesium tin halides (CsSnX3, X=Cl, Br, I) are highly desirable for substituting the organolead halide perovskite solar cells. However, the poor stability of CsSnX3 perovskites has so far prevented the fabrication of devices that can withstand sustained operation under normal conditions. In this paper, a two-step sequential deposition method is developed to grow high-quality B-gamma-CsSnI3 thin films and their unique phase change in atmosphere is explored in detail. We find the spontaneous oxidative conversion from unstable B-gamma-CsSnI3 to air-stable Cs2SnI6 in air. Allowing the phase conversion of the CsSnI3 film to evolve in ambient air it gives the semiconducting perovskite Cs2SnI6 with a bandgap of 1.48 eV and high absorption coefficient (over 10(5) cm(-1) from 1.7 eV). More importantly, the Cs2SnI6 film, for the first time, is adopted as a light absorber layer for a lead-free perovskite solar cell and a preliminary estimate of the power conversion efficiency (PCE) about 1% with open-circuit voltage of 0.51 V and short-circuit current of 5.41 mA/cm(2) is realized by optimizing the perovskite absorber thickness. According to the bandgap and the Shockley-Queisser limit, such inorganic perovskite solar cell with higher efficiency and pronounced stability can be expected by material quality improvement and device engineering. (C) 2016 Elsevier B.V. All rights reserved.
引用
收藏
页码:227 / 234
页数:8
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