In Operando, Photovoltaic, and Microscopic Evaluation of Recombination Centers in Halide Perovskite-Based Solar Cells

被引:6
作者
Zohar, Arava [1 ]
Kulbak, Michael [1 ]
Turren-Cruz, Silver H. [2 ,3 ]
Nayak, Pabitra K. [4 ,5 ]
Kama, Adi [6 ,7 ]
Hagfeldt, Anders [2 ]
Snaith, Henry J. [4 ]
Hodes, Gary [1 ]
Cahen, David [1 ,6 ,7 ]
机构
[1] Weizmann Inst Sci, Dept Mat & Interfaces, IL-76100 Rehovot, Israel
[2] Ecole Polytech Fed Lausanne, CH-1015 Lausanne, Switzerland
[3] Jaume I Univ, Inst Adv Mat INAM, Castellon de La Plana 12071, Spain
[4] Univ Oxford, Dept Phys, Clarendon Lab, Oxford OX1 3PU, England
[5] Tata Inst Fundamental Res, Hyderabad 500046, India
[6] Bar Ilan Univ, Chem Dept, IL-52900 Ramat Gan, Israel
[7] Bar Ilan Univ, Inst Nanotechnol & Adv Mat, IL-52900 Ramat Gan, Israel
关键词
defect states; diffusion length; p-i-n junction; Br-based perovskite; EBIC; ION MIGRATION; QUANTIFICATION; EFFICIENCY; DIFFUSION; DEFECTS; VOLTAGE; LIGHT;
D O I
10.1021/acsami.1c08675
中图分类号
TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
The origin of the low densities of electrically active defects in Pb halide perovskite (HaP), a crucial factor for their use in photovoltaics, light emission, and radiation detection, remains a matter of discussion, in part because of the difficulty in determining these densities. Here, we present a powerful approach to assess the defect densities, based on electric field mapping in working HaP-based solar cells. The minority carrier diffusion lengths were deduced from the electric field profile, measured by electron beam-induced current (EBIC). The EBIC method was used earlier to get the first direct evidence for the n-i-p junction structure, at the heart of efficient HaP-based PV cells, and later by us and others for further HaP studies. This manuscript includes EBIC results on illuminated cell cross sections (in operando) at several light intensities to compare optoelectronic characteristics of different cells made by different groups in several laboratories. We then apply a simple, effective single-level defect model that allows deriving the densities (N-r) of the defect acting as recombination center. We find N-r approximate to 1 x 10(13) cm(-3) for mixed A cation lead bromide-based HaP films and similar to 1 x 10(14) cm(-3) for MAPbBr(3)(Cl). As EBIC photocurrents are similar at the grain bulk and boundaries, we suggest that the defects are at the interfaces with selective contacts rather than in the HaP film. These results are relevant for photovoltaic devices as the EBIC responses distinguish clearly between high- and low-efficiency devices. The most efficient devices have n-i-p structures with a close-to-intrinsic HaP film, and the selective contacts then dictate the electric field strength throughout the HaP absorber.
引用
收藏
页码:34171 / 34179
页数:9
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