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Materials Data on CsPbCl3 by Materials Project

CsPbCl3 is (Cubic) Perovskite structured and crystallizes in the trigonal R32 space group. The structure is three-dimensional. Cs1+ is bonded in a 9-coordinate geometry to nine equivalent Cl1- atoms. There are three shorter (3.77 Å) and six longer (4.08 Å) Cs–Cl bond lengths. Pb2+ is bonded to six equivalent Cl1- atoms to form corner-sharing PbCl6 octahedra. The corner-sharing octahedral tilt angles are 11°. All Pb–Cl bond lengths are 2.88 Å. Cl1- is bonded in a 5-coordinate geometry to three equivalent Cs1+ and two equivalent Pb2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on CsPbCl3 by Materials Project

CsPbCl3 is Ilmenite-like structured and crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a 6-coordinate geometry to six Cl1- atoms. There are a spread of Cs–Cl bond distances ranging from 3.74–3.82 Å. In the second Cs1+ site, Cs1+ is bonded in a 6-coordinate geometry to six Cl1- atoms. There are four shorter (3.74 Å) and two longer (3.82 Å) Cs–Cl bond lengths. Pb2+ is bonded to six Cl1- atoms to form corner-sharing PbCl6 octahedra. The corner-sharing octahedra tilt angles range from 11–20°. There are a spread of Pb–Cl bond distances ranging from 2.88–2.92 Å. There are four inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a distorted see-saw-like geometry to two equivalent Cs1+ and two equivalent Pb2+ atoms. In the second Cl1- site, Cl1- is bonded in a distorted rectangular see-saw-like geometry to two Cs1+ and two equivalent Pb2+ atoms. In the third Cl1- site, Cl1- is bonded to two equivalent Cs1+ and two equivalent Pb2+ atoms to form distorted corner-sharing ClCs2Pb2 trigonal pyramids. In the fourth Cl1- site, Cl1- is bonded in a distorted see-saw-like geometry to two equivalent Cs1+ and two equivalent Pb2+ atoms.

36 MATERIALS SCIENCE↗

Defect Structure in Quantum-Cutting Yb3+-Doped CsPbCl3 Perovskites Probed by X-Ray Absorption and Atomic Pair Distribution Function Analysis

Ytterbium-doping in all-inorganic lead-halide perovskites (CsPb(Cl1-xBrx)3) generates novel properties including quantum cutting and narrow line emission, making these materials attractive spectral down-converters for solar photovoltaics. The relationship between this optical efficiency and the defect structure(s) associated with Yb3+ dopants within perovskites is not well understood. Various charge-neutral doping motifs have previously been proposed and studied computationally, including clusters involving two substitutional Yb3+ ions charge-compensated by a single local Pb2+ vacancy. Near-band-edge defect states associated with such motifs are believed to play an important mechanistic role in quantum cutting itself. Here, we report the results of X-ray absorption and X-ray total-scattering measurements on ytterbium-doped CsPbCl3. XANES shows that the dopant oxidation state is exclusively Yb3+, and a combination of Yb L3 and Pb L3 EXAFS shows that this Yb3+ substitutes exclusively at Pb2+ sites, where it adopts a pseudo-octahedral [YbCl6]3- coordination environment. Shell-by-shell fits to the data show a short Yb-Cl bond distance of 2.58 Å compared to the Pb-Cl bond distance of 2.83 Å. We confirm this finding by X-ray pair distribution function analysis, which also shows evidence of additional Pb2+ vacancy formation induced by Yb3+ doping. We evaluate whether this is the primary mechanism of charge compensation using simulated EXAFS and pair distribution function data for several computed defect structures. Together, these results resolve the local dopant structures and charge-compensation mechanisms in lanthanide-doped all-inorganic lead-halide perovskites, and, as such, significantly advance the understanding of structure-function relationships in this important class of materials.

Kluherz, Kyle (ORCID:0000000279865167)↗