4.8 Article

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

期刊

ACS APPLIED MATERIALS & INTERFACES
卷 14, 期 30, 页码 34171-34179

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acsami.1c08675

关键词

defect states; diffusion length; p-i-n junction; Br-based perovskite; EBIC

资金

  1. Yotam project
  2. Ullmann Family Foundation
  3. Dears Foundation
  4. WIS Sustainability And Energy Research Initiative
  5. SAERI
  6. Minerva Centre for Self-Repairing Systems for Energy Sustainability

向作者/读者索取更多资源

We present a powerful approach to assess the defect densities in lead halide perovskite materials based on electric field mapping. By measuring the electric field profile using electron beam-induced current, we deduced the defect densities and found that they mainly exist at the interfaces with selective contacts rather than in the perovskite film. These results are highly relevant for improving the efficiency of photovoltaic devices.
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.

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