Abstract

Metal halide perovskite materials (MHPs) are a family of next-generation semiconductors that are enabling low-cost, high-performance solar cells and optoelectronic devices. The most-used halogen in MHPs, iodine, can supplement its octet by covalent bonding resulting in atomic charges intermediate to I− and I0. Here, we examine theoretically stabilized defects of iodine using density functional theory (DFT); defect formation enthalpies and iodine Bader charges which illustrate how MHPs adapt to stoichiometry changes. Experimentally, X-ray photoelectron spectroscopy (XPS) is used to identify perovskite defects and their relative binding energies, and validate the predicted chemical environments of iodine defects. Examining MHP samples with excess iodine compared with near stoichiometric samples, we discern additional spectral intensity in the I 3d5/2 XPS data arising from defects, and support the presence of iodine trimers. I 3d5/2 defect peak areas reveal a ratio of 2:1, matching the number of atoms at the ends and middle of the trimer, whereas their binding energies agree with calculated Bader charges. Results suggest the iodine trimer is the preferred structural motif for incorporation of excess iodine into the perovskite lattice. Understanding these easily formed photoactive defects and how to identify their presence is essential for stabilizing MHPs against photodecomposition.

Highlights

  • IntroductionOrganometal lead halide perovskite materials (MHPs) (APbX3 where A = methylammonium MA+ , formamidinium FA+ ; X = iodide I− , bromide Br− , chloride Cl− ) have demonstrated enormous potential as high bandgap absorber layers in single-junction and tandem solar cells

  • Oxidation of iodine from I− to I0 by mixed ionic and covalent bonding is a critical factor allowing for perovskite lattice defects to form in large quantities

  • Our results show that the I− to I0 transition is responsible for electronically-active defects in MHPs which are observed using chemically sensitive X-ray photoelectron spectroscopy (XPS) measurements

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Summary

Introduction

Organometal lead halide perovskite materials (MHPs) (APbX3 where A = methylammonium MA+ , formamidinium FA+ ; X = iodide I− , bromide Br− , chloride Cl− ) have demonstrated enormous potential as high bandgap absorber layers in single-junction and tandem solar cells. Ion migration through crystallographic point defects is responsible for a wide range of phenomena in perovskite materials: current–voltage hysteresis in functional devices [3,4,5], giant photocapacitance [6,7], the light soaking effect [8,9,10], and photo-induced anion segregation [10,11,12]. Defects play an essential role in degradation of the perovskite active layer, providing a path for ion loss [13]

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