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Strain-induced structural phase transition, electric polarization and unusual electric properties in photovoltaic materials CsMI(3) (M = Pb, Sn)
The structural phase transition, ferroelectric polarization, and electric properties have been investigated for photovoltaic films CsMI(3) (M = Pb, Sn) epitaxially grown along (001) direction based on the density functional theory. The calculated results indicate that the phase diagrams of two epita...
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/PMC9051086/ https://www.ncbi.nlm.nih.gov/pubmed/35497588 http://dx.doi.org/10.1039/c9ra10791f |
Sumario: | The structural phase transition, ferroelectric polarization, and electric properties have been investigated for photovoltaic films CsMI(3) (M = Pb, Sn) epitaxially grown along (001) direction based on the density functional theory. The calculated results indicate that the phase diagrams of two epitaxial CsPbI(3) and CsSnI(3) films are almost identical, except critical transition strains varying slightly. The epitaxial tensile strains induce two ferroelectric phases Pmc2(1), and Pmn2(1), while the compressive strains drive two paraelectric phases P2(1)2(1)2(1), P2(1)2(1)2. The larger compressive strain enhances the ferroelectric instability in these two films, eventually rendering them another ferroelectric state Pc. Whether CsPbI(3) or CsSnI(3), the total polarization of Pmn2(1) phase comes from the main contribution of B-position cations (Pb or Sn), whereas, for Pmc2(1) phase, the main contributor is the I ion. Moreover, the epitaxial strain effects on antiferrodistortive vector, polarization and band gap of CsMI(3) (M = Pb, Sn) are further discussed. Unusual electronic properties under epitaxial strains are also revealed and interpreted. |
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