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Light–Induced Frenkel Defect Pair Formation Can Lead to Phase–Segregation of Otherwise Miscible Halide Perovskite Alloys

Alloys of ABX 3 halide perovskites (HP) exhibit unique phase behavior compared to traditional III-V and II-VI semiconductor alloys used in solar cells. While the latter typically have good mutual miscibility when their mixed components are size matched, and phase-segregate when size mismatched, HP alloys show good miscibility in the dark but can phase-segregate under light. Quantum mechanical calculations described herein reveal light-induced defect formation and migration hold the key. Specifically, the interaction between a halogen vacancy V X with halogen interstitial X i forming together a Frenkel-pair defect emerges as the enabler for phase-segregation in HP alloys. At a threshold bromine composition in the Br-I alloys, the photogenerated holes in the valence band localize, creating thereby a doubly-charged iodine Frenkel-pair (V I + I i ) 2+ . Faster migration of iodine over bromine interstitial into the vacant iodine V I site leads to the formation of iodine-rich and iodine-depleted regions, establishing phase-segregation. Removal of the mobile defects–the agent of segregation–by dark thermal annealing, supplies the opposing force, leading to reversal of phase-segregation. Furthermore, this atomistic understanding can enable some control of the phase-segregation by selecting substituting elements on the B site–such as replacing some Pb by Sn–that are unable to form stable Frenkel defects.

14 SOLAR ENERGY↗

Materials Data on IBr by Materials Project

IBr crystallizes in the orthorhombic Cmcm space group. The structure is one-dimensional and consists of two IBr ribbons oriented in the (0, 0, 1) direction. I is bonded in a linear geometry to two equivalent Br atoms. Both I–Br bond lengths are 2.73 Å. Br is bonded in a water-like geometry to two equivalent I atoms.

36 MATERIALS SCIENCE↗

Materials Data on YBr3 by Materials Project

YBr3 is Aluminum trichloride structured and crystallizes in the monoclinic C2/m space group. The structure is two-dimensional and consists of one YBr3 sheet oriented in the (0, 0, 1) direction. Y3+ is bonded to six Br1- atoms to form edge-sharing YBr6 octahedra. All Y–Br bond lengths are 2.82 Å. There are two inequivalent Br1- sites. In the first Br1- site, Br1- is bonded in an L-shaped geometry to two equivalent Y3+ atoms. In the second Br1- site, Br1- is bonded in an L-shaped geometry to two equivalent Y3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on YBr3 by Materials Project

YBr3 crystallizes in the hexagonal P6_3/mmc space group. The structure is one-dimensional and consists of two YBr3 ribbons oriented in the (0, 0, 1) direction. Y3+ is bonded to six equivalent Br1- atoms to form distorted face-sharing YBr6 pentagonal pyramids. All Y–Br bond lengths are 2.83 Å. Br1- is bonded in an L-shaped geometry to two equivalent Y3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y2Br3 by Materials Project

Y2Br3 crystallizes in the monoclinic C2/m space group. The structure is two-dimensional and consists of one Y2Br3 sheet oriented in the (2, 0, -1) direction. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 4-coordinate geometry to four Br atoms. There are two shorter (2.91 Å) and two longer (2.93 Å) Y–Br bond lengths. In the second Y site, Y is bonded in a pentagonal planar geometry to five Br atoms. There are a spread of Y–Br bond distances ranging from 2.89–3.03 Å. There are three inequivalent Br sites. In the first Br site, Br is bonded in a trigonal non-coplanar geometry to three equivalent Y atoms. In the second Br site, Br is bonded in a distorted T-shaped geometry to three Y atoms. In the third Br site, Br is bonded in a distorted T-shaped geometry to three Y atoms.

36 MATERIALS SCIENCE↗