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Unexpected bowing band evolution in an all-inorganic CsSn(1−x)Pb(x)Br(3) perovskite
We theoretically investigated the structural and electronic properties of the all-inorganic perovskite CsSn(1−x)Pb(x)Br(3), compared with the mixed perovskite compound MA(y)Cs(1−y)Sn(1−x)Pb(x)Br(3), based on first-principle calculations. It has been demonstrated that Pb and Sn atoms are inclined to...
Autores principales: | , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9055386/ https://www.ncbi.nlm.nih.gov/pubmed/35519736 http://dx.doi.org/10.1039/d0ra03709e |
Sumario: | We theoretically investigated the structural and electronic properties of the all-inorganic perovskite CsSn(1−x)Pb(x)Br(3), compared with the mixed perovskite compound MA(y)Cs(1−y)Sn(1−x)Pb(x)Br(3), based on first-principle calculations. It has been demonstrated that Pb and Sn atoms are inclined to occupy the lattice sites uniformly in the all-inorganic perovskite, and this is distinguished from the most stable configurations observed in the mixed Cs-MA system. It is interesting that small Sn atoms prefer to stay close to the large MA(+) cations, leading to smaller local structural distortion. Through spin-orbital coupling calculations, we found non-linear bowing band evolution in the all-inorganic mixed Sn–Pb system with a small bowing parameter (b = 0.35), while the band gap of MA(y)Cs(1−y)Sn(1−x)Pb(x)Br(3) was clearly reduced as the ratio of MA was around 0.5 (y ≥ 0.25). We determined the bowing band evolution in the mixed cation perovskites and the intrinsic electronic deficiency of the all-inorganic perovskite to obtain the optimal band gap. |
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