Cargando…
Preferred oriented cation configurations in high pressure phases IV and V of methylammonium lead iodide perovskite
A microscopic viewpoint of structure and dipolar configurations in hybrid organic–inorganic perovskites is crucial to understanding their stability and phase transitions. The necessity of incorporating dispersion interactions in the state-of-the-art density functional theory for the [Formula: see te...
Autores principales: | , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2020
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7713306/ https://www.ncbi.nlm.nih.gov/pubmed/33273554 http://dx.doi.org/10.1038/s41598-020-77852-y |
_version_ | 1783618552269373440 |
---|---|
author | Sukmas, Wiwittawin Sakulsupich, Vichawan Tsuppayakorn-aek, Prutthipong Pinsook, Udomsilp Pakornchote, Teerachote Klinkla, Rakchat Bovornratanaraks, Thiti |
author_facet | Sukmas, Wiwittawin Sakulsupich, Vichawan Tsuppayakorn-aek, Prutthipong Pinsook, Udomsilp Pakornchote, Teerachote Klinkla, Rakchat Bovornratanaraks, Thiti |
author_sort | Sukmas, Wiwittawin |
collection | PubMed |
description | A microscopic viewpoint of structure and dipolar configurations in hybrid organic–inorganic perovskites is crucial to understanding their stability and phase transitions. The necessity of incorporating dispersion interactions in the state-of-the-art density functional theory for the [Formula: see text] perovskite (MAPI) is demonstrated in this work. Some of the vdW methods were selected to evaluate the corresponding energetics properties of the cubic MAPI with various azimuthally rotated MA organic cation orientations. The highest energy barrier obtained from PBEsol reaches 18.6 meV/MA-ion, which is equivalent to 216 K, the temperature above which the MA cations randomly reorient. Energy profiles calculated by vdW incorporated functionals, on the other hand, exhibit various distinct patterns. The well-developed vdW-DF-cx functional was selected, thanks to its competence, to evaluate the total energies of different MA dipolar configurations in [Formula: see text] cubic supercell of MAPI under pressures. The centrosymmetric arrangement of the MA cations that provide zero total dipole moment configuration results in the lowest energy state profiles under pressure, while the non-centrosymmetric scheme displays a unique behaviour. Despite being overall unpolarised, the latter calculated with PBEsol leads to a rigid shift of energy from the profile obtained from the dispersive vdW-DF-cx functional. It is noteworthy that the energy profile responsible for the maximum polarised configuration nevertheless takes the second place in total energy under pressure. |
format | Online Article Text |
id | pubmed-7713306 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-77133062020-12-03 Preferred oriented cation configurations in high pressure phases IV and V of methylammonium lead iodide perovskite Sukmas, Wiwittawin Sakulsupich, Vichawan Tsuppayakorn-aek, Prutthipong Pinsook, Udomsilp Pakornchote, Teerachote Klinkla, Rakchat Bovornratanaraks, Thiti Sci Rep Article A microscopic viewpoint of structure and dipolar configurations in hybrid organic–inorganic perovskites is crucial to understanding their stability and phase transitions. The necessity of incorporating dispersion interactions in the state-of-the-art density functional theory for the [Formula: see text] perovskite (MAPI) is demonstrated in this work. Some of the vdW methods were selected to evaluate the corresponding energetics properties of the cubic MAPI with various azimuthally rotated MA organic cation orientations. The highest energy barrier obtained from PBEsol reaches 18.6 meV/MA-ion, which is equivalent to 216 K, the temperature above which the MA cations randomly reorient. Energy profiles calculated by vdW incorporated functionals, on the other hand, exhibit various distinct patterns. The well-developed vdW-DF-cx functional was selected, thanks to its competence, to evaluate the total energies of different MA dipolar configurations in [Formula: see text] cubic supercell of MAPI under pressures. The centrosymmetric arrangement of the MA cations that provide zero total dipole moment configuration results in the lowest energy state profiles under pressure, while the non-centrosymmetric scheme displays a unique behaviour. Despite being overall unpolarised, the latter calculated with PBEsol leads to a rigid shift of energy from the profile obtained from the dispersive vdW-DF-cx functional. It is noteworthy that the energy profile responsible for the maximum polarised configuration nevertheless takes the second place in total energy under pressure. Nature Publishing Group UK 2020-12-03 /pmc/articles/PMC7713306/ /pubmed/33273554 http://dx.doi.org/10.1038/s41598-020-77852-y Text en © The Author(s) 2020 Open AccessThis article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/. |
spellingShingle | Article Sukmas, Wiwittawin Sakulsupich, Vichawan Tsuppayakorn-aek, Prutthipong Pinsook, Udomsilp Pakornchote, Teerachote Klinkla, Rakchat Bovornratanaraks, Thiti Preferred oriented cation configurations in high pressure phases IV and V of methylammonium lead iodide perovskite |
title | Preferred oriented cation configurations in high pressure phases IV and V of methylammonium lead iodide perovskite |
title_full | Preferred oriented cation configurations in high pressure phases IV and V of methylammonium lead iodide perovskite |
title_fullStr | Preferred oriented cation configurations in high pressure phases IV and V of methylammonium lead iodide perovskite |
title_full_unstemmed | Preferred oriented cation configurations in high pressure phases IV and V of methylammonium lead iodide perovskite |
title_short | Preferred oriented cation configurations in high pressure phases IV and V of methylammonium lead iodide perovskite |
title_sort | preferred oriented cation configurations in high pressure phases iv and v of methylammonium lead iodide perovskite |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7713306/ https://www.ncbi.nlm.nih.gov/pubmed/33273554 http://dx.doi.org/10.1038/s41598-020-77852-y |
work_keys_str_mv | AT sukmaswiwittawin preferredorientedcationconfigurationsinhighpressurephasesivandvofmethylammoniumleadiodideperovskite AT sakulsupichvichawan preferredorientedcationconfigurationsinhighpressurephasesivandvofmethylammoniumleadiodideperovskite AT tsuppayakornaekprutthipong preferredorientedcationconfigurationsinhighpressurephasesivandvofmethylammoniumleadiodideperovskite AT pinsookudomsilp preferredorientedcationconfigurationsinhighpressurephasesivandvofmethylammoniumleadiodideperovskite AT pakornchoteteerachote preferredorientedcationconfigurationsinhighpressurephasesivandvofmethylammoniumleadiodideperovskite AT klinklarakchat preferredorientedcationconfigurationsinhighpressurephasesivandvofmethylammoniumleadiodideperovskite AT bovornratanaraksthiti preferredorientedcationconfigurationsinhighpressurephasesivandvofmethylammoniumleadiodideperovskite |