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Effect of Dimensionality on Photoluminescence and Dielectric Properties of Imidazolium Lead Bromides

[Image: see text] Hybrid organic–inorganic lead halide perovskites have emerged as promising materials for various applications, including solar cells, light-emitting devices, dielectrics, and optical switches. In this work, we report the synthesis, crystal structures, and linear and nonlinear optic...

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Detalles Bibliográficos
Autores principales: Smółka, Szymon, Mączka, Mirosław, Drozdowski, Dawid, Stefańska, Dagmara, Gągor, Anna, Sieradzki, Adam, Zaręba, Jan K., Ptak, Maciej
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9516686/
https://www.ncbi.nlm.nih.gov/pubmed/36102245
http://dx.doi.org/10.1021/acs.inorgchem.2c02496
Descripción
Sumario:[Image: see text] Hybrid organic–inorganic lead halide perovskites have emerged as promising materials for various applications, including solar cells, light-emitting devices, dielectrics, and optical switches. In this work, we report the synthesis, crystal structures, and linear and nonlinear optical as well as dielectric properties of three imidazolium lead bromides, IMPbBr(3), IM(2)PbBr(4), and IM(3)PbBr(5) (IM(+) = imidazolium). We show that these compounds exhibit three distinct structure types. IMPbBr(3) crystallizes in the 4H-hexagonal perovskite structure with face- and corner-shared PbBr(6) octahedra (space group P6(3)/mmc at 295 K), IM(2)PbBr(4) adopts a one-dimensional (1D) double-chain structure with edge-shared octahedra (space group P1̅ at 295 K), while IM(3)PbBr(5) crystallizes in the 1D single-chain structure with corner-shared PbBr(6) octahedra (space group P1̅ at 295 K). All compounds exhibit two structural phase transitions, and the lowest temperature phases of IMPbBr(3) and IM(3)PbBr(5) are noncentrosymmetric (space groups Pna2(1) at 190 K and P1 at 100 K, respectively), as confirmed by measurements of second-harmonic generation (SHG) activity. X-ray diffraction and thermal and Raman studies demonstrate that the phase transitions feature an order–disorder mechanism. The only exception is the isostructural P1̅ to P1̅ phase transition at 141 K in IM(2)PbBr(4), which is of a displacive type. Dielectric studies reveal that IMPbBr(3) is a switchable dielectric material, whereas IM(3)PbBr(5) is an improper ferroelectric. All compounds exhibit broadband, highly shifted Stokes emissions. Features of these emissions, i.e., band gap and excitonic absorption, are discussed in relation to the different structures of each composition.