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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...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2021
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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 |
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. |
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