Abstract

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 (Nr) of the defect acting as recombination center. We find Nr ≈ 1 × 1013 cm-3 for mixed A cation lead bromide-based HaP films and ∼1 × 1014 cm-3 for MAPbBr3(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.

Highlights

  • Halide perovskites (HaPs), those containing lead, have properties of high-quality semiconductor materials suitable for a solar cell application, especially because their preparation procedure requires low energy consumption

  • We have argued that the crucial property that allows the phenomenal performance of lead HaP-based PV cells is the low defect density and/or the low optoelectronic activity of such defects.[5,6]

  • The right solar cell is a Br-based HaP sandwiched between FTO/d-TiO2 mp-TiO2 and PTAA/Au

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Summary

■ INTRODUCTION

Halide perovskites (HaPs), those containing lead, have properties of high-quality semiconductor materials suitable for a solar cell application, especially because their preparation procedure requires low energy consumption (low temperatures, atmospheric pressure). Profiles of the EBIC signal in all cases show similar widths that are matched to the thickness of the HaP film This suggests that the MAPI-based solar cell retained its n-i-p character, because of photogeneration, the free electron and hole concentrations are orders of magnitude higher than in the dark, and this increases the importance of interface defects. Such a profile implies that the LD is greater than the film thickness, and in such a case, we cannot determine from EBIC how it changes as a function of illumination, as we only can give a lower estimate of LD.

■ CONCLUSIONS
■ ACKNOWLEDGMENTS
■ REFERENCES
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