Cargando…
Multi Band Gap Electronic Structure in CH(3)NH(3)PbI(3)
Organo-lead halide perovskite solar cells represent a revolutionary shift in solar photovoltaics, introducing relatively soft defect containing semiconductors as materials with excellent charge collection for both electrons and holes. Although they are based on the nominally simple cubic perovskite...
Autores principales: | , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2019
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6376135/ https://www.ncbi.nlm.nih.gov/pubmed/30765739 http://dx.doi.org/10.1038/s41598-018-38023-2 |
_version_ | 1783395499962793984 |
---|---|
author | Ong, Khuong P. Wu, Shunnian Nguyen, Tien Hoa Singh, David J. Fan, Zhen Sullivan, Michael B. Dang, Cuong |
author_facet | Ong, Khuong P. Wu, Shunnian Nguyen, Tien Hoa Singh, David J. Fan, Zhen Sullivan, Michael B. Dang, Cuong |
author_sort | Ong, Khuong P. |
collection | PubMed |
description | Organo-lead halide perovskite solar cells represent a revolutionary shift in solar photovoltaics, introducing relatively soft defect containing semiconductors as materials with excellent charge collection for both electrons and holes. Although they are based on the nominally simple cubic perovskite structure, these compounds are in fact very complex. For example, in (CH(3)NH(3))PbI(3) the dynamics and ensuing structural fluctuations associated with the (CH(3)NH(3))(+) ions and the interplay with the electronic properties are still not fully understood, despite extensive study. Here, using ab-initio calculations, we show that at room and higher temperature, the rotation of CH(3)NH(3) molecules can be viewed as effectively giving local structures that are cubic and tetragonal like from the point of view of the PbI(3) framework, though in fact having lower symmetry. Both of these structures are locally polar, with sizable polarization, ~10 μC/cm(2) due to the dipoles on the organic. They become energetically degenerate in the volume range, V ~ 250 Å(3)/f.u–265 Å(3)/f.u. We also find very significant dependence of the band gap on the local structure. This type of transition is analogous to a transition between two ferroelectric structures, where in-spite of strong electron phonon coupling, there is strong screening of charged defects which can lead to enhanced mobility and charge collection. The results provide insights into the enhanced light absorption near the band edge and good charge collection in this material. |
format | Online Article Text |
id | pubmed-6376135 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-63761352019-02-19 Multi Band Gap Electronic Structure in CH(3)NH(3)PbI(3) Ong, Khuong P. Wu, Shunnian Nguyen, Tien Hoa Singh, David J. Fan, Zhen Sullivan, Michael B. Dang, Cuong Sci Rep Article Organo-lead halide perovskite solar cells represent a revolutionary shift in solar photovoltaics, introducing relatively soft defect containing semiconductors as materials with excellent charge collection for both electrons and holes. Although they are based on the nominally simple cubic perovskite structure, these compounds are in fact very complex. For example, in (CH(3)NH(3))PbI(3) the dynamics and ensuing structural fluctuations associated with the (CH(3)NH(3))(+) ions and the interplay with the electronic properties are still not fully understood, despite extensive study. Here, using ab-initio calculations, we show that at room and higher temperature, the rotation of CH(3)NH(3) molecules can be viewed as effectively giving local structures that are cubic and tetragonal like from the point of view of the PbI(3) framework, though in fact having lower symmetry. Both of these structures are locally polar, with sizable polarization, ~10 μC/cm(2) due to the dipoles on the organic. They become energetically degenerate in the volume range, V ~ 250 Å(3)/f.u–265 Å(3)/f.u. We also find very significant dependence of the band gap on the local structure. This type of transition is analogous to a transition between two ferroelectric structures, where in-spite of strong electron phonon coupling, there is strong screening of charged defects which can lead to enhanced mobility and charge collection. The results provide insights into the enhanced light absorption near the band edge and good charge collection in this material. Nature Publishing Group UK 2019-02-14 /pmc/articles/PMC6376135/ /pubmed/30765739 http://dx.doi.org/10.1038/s41598-018-38023-2 Text en © The Author(s) 2019 Open Access This 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 license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license 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 license, visit http://creativecommons.org/licenses/by/4.0/. |
spellingShingle | Article Ong, Khuong P. Wu, Shunnian Nguyen, Tien Hoa Singh, David J. Fan, Zhen Sullivan, Michael B. Dang, Cuong Multi Band Gap Electronic Structure in CH(3)NH(3)PbI(3) |
title | Multi Band Gap Electronic Structure in CH(3)NH(3)PbI(3) |
title_full | Multi Band Gap Electronic Structure in CH(3)NH(3)PbI(3) |
title_fullStr | Multi Band Gap Electronic Structure in CH(3)NH(3)PbI(3) |
title_full_unstemmed | Multi Band Gap Electronic Structure in CH(3)NH(3)PbI(3) |
title_short | Multi Band Gap Electronic Structure in CH(3)NH(3)PbI(3) |
title_sort | multi band gap electronic structure in ch(3)nh(3)pbi(3) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6376135/ https://www.ncbi.nlm.nih.gov/pubmed/30765739 http://dx.doi.org/10.1038/s41598-018-38023-2 |
work_keys_str_mv | AT ongkhuongp multibandgapelectronicstructureinch3nh3pbi3 AT wushunnian multibandgapelectronicstructureinch3nh3pbi3 AT nguyentienhoa multibandgapelectronicstructureinch3nh3pbi3 AT singhdavidj multibandgapelectronicstructureinch3nh3pbi3 AT fanzhen multibandgapelectronicstructureinch3nh3pbi3 AT sullivanmichaelb multibandgapelectronicstructureinch3nh3pbi3 AT dangcuong multibandgapelectronicstructureinch3nh3pbi3 |