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Lead-free hybrid perovskite N(CH(3))(4)SnI(3) with robust ferroelectricity induced by large and non-polar N(CH(3))(4)(+) molecular cation

The ferroelectricity in the hybrid perovskite CH(3)NH(3)PbI(3) is under debate because it results from the polar molecular cation CH(3)NH(3)(+) while the molecular orientation was reported to be random. Here we predict that a Pb-free hybrid perovskite N(CH(3))(4)SnI(3) with non-polar molecular catio...

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Detalles Bibliográficos
Autores principales: Wei, Hai, Yang, Yali, Chen, Shiyou, Xiang, H. J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7840759/
https://www.ncbi.nlm.nih.gov/pubmed/33504812
http://dx.doi.org/10.1038/s41467-021-20889-y
Descripción
Sumario:The ferroelectricity in the hybrid perovskite CH(3)NH(3)PbI(3) is under debate because it results from the polar molecular cation CH(3)NH(3)(+) while the molecular orientation was reported to be random. Here we predict that a Pb-free hybrid perovskite N(CH(3))(4)SnI(3) with non-polar molecular cation N(CH(3))(4)(+) has strong ferroelectricity with a spontaneous polarization of 16.13 μC cm(−2). The large polarization results from the distortion of SnI(6) octahedron induced by the large N(CH(3))(4)(+) and is independent of the molecular orientation, so the ferroelectricity is robust. The ferroelectric R3m perovskite structure of N(CH(3))(4)SnI(3) can be synthesized as the ground state under a hydrostatic pressure over 3 GPa and remains stable under ambient pressure. Given the strong ferroelectricity, good stability and high visible-light absorption, N(CH(3))(4)SnI(3) may be an ideal light-absorber semiconductor for high-efficiency solar cells because its ferroelectric polarization can facilitate electron-hole separation and produce large bulk photovoltaic effect, making the design of homogeneous bulk photovoltaic devices possible.