Lattice Distortion in Mixed-Anion Lead Halide Perovskite Nanorods Leads to their High Fluorescence Anisotropy AITranslate
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Semiconductor nanorods (NRs) with strong fluorescence anisotropy are considered promising polarized light sources for liquid crystal displays. Here, we achieved a high fluorescence anisotropy value of 0.4 in the mixed-anion lead halide perovskite NRs, which constitutes a four-fold enhancement as compared to pristine CsPbBr3 NRs. This was realized by substituting some smaller bromine anions with larger iodine anions in the orthorhombic CsPbBr3 NRs via anion exchange. The resulting CsPbBr1.2I1.8 NRs kept a highly uniform length of ∼36 nm and width of ∼8.6 nm, and possessed a high emission quantum yield of 83%. On the basis of the DFT calculations, we attribute the improved polarized emission of the mixed-anion perovskite NRs to a moderate structural distortion of PbX6 octahedra units in the orthorhombic perovskite lattice, which results in a preferred direction of the optical transition dipole moment along the Pb–X–Pb axis. Our study provides a guidance for design and fabrication of perovskite NRs with high fluorescence anisotropy.
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DOI:https://doi.org/10.1021/acsmaterialslett.0c00118
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Semiconductor nanorods (NRs) with strong fluorescence anisotropy are considered promising polarized light sources for liquid crystal displays. Here, we achieved a high fluorescence anisotropy value of 0.4 in the mixed-anion lead halide perovskite NRs, which constitutes a four-fold enhancement as compared to pristine CsPbBr3 NRs. This was realized by substituting some smaller bromine anions with larger iodine anions in the orthorhombic CsPbBr3 NRs via anion exchange. The resulting CsPbBr1.2I1.8 NRs kept a highly uniform length of ∼36 nm and width of ∼8.6 nm, and possessed a high emission quantum yield of 83%. On the basis of the DFT calculations, we attribute the improved polarized emission of the mixed-anion perovskite NRs to a moderate structural distortion of PbX6 octahedra units in the orthorhombic perovskite lattice, which results in a preferred direction of the optical transition dipole moment along the Pb–X–Pb axis. Our study provides a guidance for design and fabrication of perovskite NRs with high fluorescence anisotropy.
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| GB/T 7714-2015 | [1] Yongjiang Dou, Fan Cao, Tetiana Dudka, et al. ACS Materials Letters, 2020(2). DOI:10.1021/acsmaterialslett.0c00118. |
| MLA | [1] Yongjiang Dou, et al., ACS Materials Letters, no. 2, 2020, https://doi.org/10.1021/acsmaterialslett.0c00118. |
| APA | [1] Yongjiang Dou, Fan Cao, Tetiana Dudka, Yunguo Li, Sheng Wang, Chengxi Zhang, Yuan Gao, Xuyong Yang, & Andrey L. Rogach. (2020). ACS Materials Letters(2). https://doi.org/10.1021/acsmaterialslett.0c00118 |
| IEEE | [1] Yongjiang Dou, Fan Cao, Tetiana Dudka, Yunguo Li, Sheng Wang, Chengxi Zhang, Yuan Gao, Xuyong Yang, and Andrey L. Rogach, ACS Materials Letters, no. 2, 2020, doi: 10.1021/acsmaterialslett.0c00118. |
