Static Rashba Effect by Surface Reconstruction and Photon Recycling in the Dynamic Indirect Gap of APbBr3 (A = Cs, CH3NH3) Single Crystals
- Hongsun Ryu ,
- Dae Young ParkDae Young ParkDepartment of Energy Science, Sungkyunkwan University, Suwon 16419, South KoreaMore by Dae Young Park,
- Kyle M. McCallKyle M. McCallDepartment of Chemistry, Northwestern University, Evanston, Illinois 60208, United StatesLaboratory of Inorganic Chemistry, Department of Chemistry and Applied Biosciences, ETH Zurich, Zurich 8093, SwitzerlandLaboratory for Thin Films and Photovoltaics, Empa-Swiss Federal Laboratories for Materials Science and Technology, Dübendorf CH-8600, SwitzerlandMore by Kyle M. McCall,
- Hye Ryung ByunHye Ryung ByunDepartment of Physics, Sogang University, Seoul 04107, South KoreaMore by Hye Ryung Byun,
- Yongjun LeeYongjun LeeDepartment of Energy Science, Sungkyunkwan University, Suwon 16419, South KoreaMore by Yongjun Lee,
- Tae Jung KimTae Jung KimDepartment of Physics, Kyung Hee University, Seoul 02447, South KoreaMore by Tae Jung Kim,
- Mun Seok JeongMun Seok JeongDepartment of Energy Science, Sungkyunkwan University, Suwon 16419, South KoreaMore by Mun Seok Jeong,
- Jeongyong KimJeongyong KimDepartment of Energy Science, Sungkyunkwan University, Suwon 16419, South KoreaMore by Jeongyong Kim,
- Mercouri G. KanatzidisMercouri G. KanatzidisDepartment of Chemistry, Northwestern University, Evanston, Illinois 60208, United StatesMore by Mercouri G. Kanatzidis, and
- Joon I. Jang*Joon I. Jang*Email: [email protected]Department of Physics, Sogang University, Seoul 04107, South KoreaMore by Joon I. Jang
Abstract

Recently, halide perovskites have gained significant attention from the perspective of efficient spintronics owing to the Rashba effect. This effect occurs as a consequence of strong spin–orbit coupling under a noncentrosymmetric environment, which can be dynamic and/or static. However, there exist intense debates on the origin of broken inversion symmetry since the halide perovskites typically crystallize into a centrosymmetric structure. In order to clarify the issue, we examine both dynamic and static effects in the all-inorganic CsPbBr3 and organic–inorganic CH3NH3PbBr3 (MAPbBr3) perovskite single crystals by employing temperature- and polarization-dependent photoluminescence excitation spectroscopy. The perovskite single crystals manifest the dynamic effect by photon recycling in the indirect Rashba gap, causing dual peaks in the photoluminescence. However, the effect vanishes in CsPbBr3 at low temperatures (<50 K) accompanied by a striking color change of the crystal, arising presumably from lower degrees of freedom for inversion symmetry breaking associated with the thermal motion of the spherical Cs cation compared with the polar MA cation in MAPbBr3. We also show that the static Rashba effect occurs only in MAPbBr3 below 90 K, presumably due to surface reconstruction via MA-cation ordering, which likely extends across a few layers from the crystal surface to the interior. We further demonstrate that this static Rashba effect can be completely suppressed upon surface treatment with polymethyl methacrylate (PMMA) coating. We believe that our results provide a rationale for the Rashba effects in halide perovskites.
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This article is cited by 9 publications.
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