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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...

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Detalles Bibliográficos
Autores principales: Xia, Yufan, Chen, Yuxuan, Luo, Tian, Liang, Hongyao, Gao, Yujia, Xu, Xin, Xie, Weiguang, Liu, Pengyi, Wang, Xin, Zhao, Yu-Jun, Shi, Tingting
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2020
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
Descripción
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.