Chiral metal halides are promising materials for nonlinear optics and spin-selective devices. Typically, chirality is introduced via large chiral organic cations, leading to low-dimensional structures and limitations in charge transport. Here, we design a family of chiral metal halides based on the relatively small ditopic R/S-3-aminoquinuclidine (3-AQ) cation, forming an (R/S-3AQ)Pb2Br6 structure closely related to the 3D corner-sharing octahedral network of perovskites. The resulting material exhibits a direct bandgap, isotropic band structure, and fully 3D photoexcitation. Circular dichroism confirms a chiral anisotropy factor consistent with theoretical predictions. Moreover, the material displays a Rashba effect in the conduction band, which is attributed to spin-orbit coupling and the lack of inversion symmetry. Offering rich chemical tunability and efficient 3D charge transport, this new class of chiral semiconductors provides a promising platform for advancing nonlinear optoelectronic and spintronic devices.
3D Chiral Metal Halide Semiconductors / Moroni, Marco; Gregori, Luca; Coccia, Clarissa; Boiocchi, Massimo; Morana, Marta; Capsoni, Doretta; Olivati, Andrea; Treglia, Antonella; Folpini, Giulia; Patrini, Maddalena; Goncalves, Isabel; Wang, Heyong; Milanese, Chiara; Petrozza, Annamaria; Mosconi, Edoardo; De Angelis, Filippo; Malavasi, Lorenzo. - In: ACS ENERGY LETTERS. - ISSN 2380-8195. - ELETTRONICO. - 10:(2025), pp. 2906-2912. [10.1021/acsenergylett.5c00576]
3D Chiral Metal Halide Semiconductors
Morana, Marta;
2025
Abstract
Chiral metal halides are promising materials for nonlinear optics and spin-selective devices. Typically, chirality is introduced via large chiral organic cations, leading to low-dimensional structures and limitations in charge transport. Here, we design a family of chiral metal halides based on the relatively small ditopic R/S-3-aminoquinuclidine (3-AQ) cation, forming an (R/S-3AQ)Pb2Br6 structure closely related to the 3D corner-sharing octahedral network of perovskites. The resulting material exhibits a direct bandgap, isotropic band structure, and fully 3D photoexcitation. Circular dichroism confirms a chiral anisotropy factor consistent with theoretical predictions. Moreover, the material displays a Rashba effect in the conduction band, which is attributed to spin-orbit coupling and the lack of inversion symmetry. Offering rich chemical tunability and efficient 3D charge transport, this new class of chiral semiconductors provides a promising platform for advancing nonlinear optoelectronic and spintronic devices.| File | Dimensione | Formato | |
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