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Bandgap Pressure Coefficient of a CH(3)NH(3)PbI(3) Thin Film Perovskite

[Image: see text] Recent scientific interest in examining the bandgap evolution of a MAPbI(3) hybrid perovskite by applying hydrostatic pressure has mostly focused on a room-temperature tetragonal phase. In contrast, the pressure response of a low-temperature orthorhombic phase (OP) of MAPbI(3) has...

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Detalles Bibliográficos
Autores principales: Pienia̧żek, Agnieszka, Dybała, Filip, Polak, Maciej P., Przypis, Łukasz, Herman, Artur P., Kopaczek, Jan, Kudrawiec, Robert
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10364135/
https://www.ncbi.nlm.nih.gov/pubmed/37436849
http://dx.doi.org/10.1021/acs.jpclett.3c01258
Descripción
Sumario:[Image: see text] Recent scientific interest in examining the bandgap evolution of a MAPbI(3) hybrid perovskite by applying hydrostatic pressure has mostly focused on a room-temperature tetragonal phase. In contrast, the pressure response of a low-temperature orthorhombic phase (OP) of MAPbI(3) has not been explored and understood. In this research, we investigate for the first time how hydrostatic pressure alters the electronic landscape of the OP of MAPbI(3). Pressure studies using photoluminescence combined with calculations within density functional theory at zero temperature allowed us to identify the main physical factors affecting the bandgap evolution of the OP of MAPbI(3). The negative bandgap pressure coefficient was found to be strongly dependent on the temperature (α(120K) = −13.3 ± 0.1 meV/GPa, α(80K) = −29.8 ± 0.1 meV/GPa, and α(40K) = −36.3 ± 0.1 meV/GPa). Such dependence is related to the changes in the Pb–I bond length and geometry in the unit cell as the atomic configuration approaches the phase transition as well as the increasing phonon contribution to octahedral tilting as the temperature increases.