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Polymer‐Passivated Inorganic Cesium Lead Mixed‐Halide Perovskites for Stable and Efficient Solar Cells with High Open‐Circuit Voltage over 1.3 V
Author(s) -
Zeng Qingsen,
Zhang Xiaoyu,
Feng Xiaolei,
Lu Siyu,
Chen Zhaolai,
Yong Xue,
Redfern Simon A. T.,
Wei Haotong,
Wang Haiyu,
Shen Huaizhong,
Zhang Wei,
Zheng Weitao,
Zhang Hao,
Tse John S.,
Yang Bai
Publication year - 2018
Publication title -
advanced materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 10.707
H-Index - 527
eISSN - 1521-4095
pISSN - 0935-9648
DOI - 10.1002/adma.201705393
Subject(s) - materials science , halide , caesium , open circuit voltage , perovskite (structure) , polymer , lead (geology) , inorganic chemistry , voltage , chemical engineering , optoelectronics , composite material , electrical engineering , chemistry , engineering , geomorphology , geology
Cesium‐based trihalide perovskites have been demonstrated as promising light absorbers for photovoltaic applications due to their superb composition stability. However, the large energy losses ( E loss ) observed in inorganic perovskite solar cells has become a major hindrance impairing the ultimate efficiency. Here, an effective and reproducible method of modifying the interface between a CsPbI 2 Br absorber and polythiophene hole‐acceptor to minimize the E loss is reported. It is demonstrated that polythiophene, deposited on the top of CsPbI 2 Br, can significantly reduce electron‐hole recombination within the perovskite, which is due to the electronic passivation of surface defect states. In addition, the interfacial properties are improved by a simple annealing process, leading to significantly reduced energy disorder in polythiophene and enhanced hole‐injection into the hole‐acceptor. Consequently, one of the highest power conversion efficiency (PCE) of 12.02% from a reverse scan in inorganic mixed‐halide perovskite solar cells is obtained. Modifying the perovskite films with annealing polythiophene enables an open‐circuit voltage ( V OC ) of up to 1.32 V and E loss of down to 0.5 eV, which both are the optimal values reported among cesium‐lead mixed‐halide perovskite solar cells to date. This method provides a new route to further improve the efficiency of perovskite solar cells by minimizing the E loss .