Cargando…
Electrical transport properties of TiO(2)/MAPbI(3) and SnO(2)/MAPbI(3) heterojunction interfaces under high pressure
The electrical transport properties of SnO(2)(TiO(2))/MAPbI(3) (MA = CH(3)NH(3)(+)) heterojunction interfaces are investigated from ambient pressure to 20 GPa, and the transport properties are calculated by physical parameters such as trap energy density, binding energy, and charge transfer driving...
Autores principales: | , , , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2023
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9869466/ https://www.ncbi.nlm.nih.gov/pubmed/36756422 http://dx.doi.org/10.1039/d2ra08143a |
_version_ | 1784876774575833088 |
---|---|
author | Li, Yuqiang Li, Yuhong Zhang, Qiang Liu, Xiaofeng Li, Yuanjing Xiao, Ningru Ning, Pingfan Wang, Jingjing Zhang, Jianxin Liu, Hongwei |
author_facet | Li, Yuqiang Li, Yuhong Zhang, Qiang Liu, Xiaofeng Li, Yuanjing Xiao, Ningru Ning, Pingfan Wang, Jingjing Zhang, Jianxin Liu, Hongwei |
author_sort | Li, Yuqiang |
collection | PubMed |
description | The electrical transport properties of SnO(2)(TiO(2))/MAPbI(3) (MA = CH(3)NH(3)(+)) heterojunction interfaces are investigated from ambient pressure to 20 GPa, and the transport properties are calculated by physical parameters such as trap energy density, binding energy, and charge transfer driving force and defect. Based on the partial density of states (PDOS) of the SnO(2)/MAPbI(3) heterojunction interface MAI-termination and PbI(2)-termination, greater charge transfer driving force and higher binding energy are observed, obviously showing the SnO(2)-based heterojunction is more stable. The SnO(2)/MAPbI(3) heterojunction interface possesses stronger electrical transport ability and is less prone to capture electrons compared with the TiO(2)/MAPbI(3) heterojunction interface. The differential charge density spectrum shows that the density is lower in the trap energy level of SnO(2)/MAPbI(3), whilst the effect of the charge transfer defect is weaker owing to the trap energy level only existing in SnO(2). The SnO(2)/MAPbI(3) heterostructure interface is less prone to capture electrons. The greater electron concentration difference is attributed to oxygen vacancy (Vo(0)) in the SnO-like environment, resulting in superior electron transport ability compared with the TiO-like environment. |
format | Online Article Text |
id | pubmed-9869466 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | The Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
spelling | pubmed-98694662023-02-07 Electrical transport properties of TiO(2)/MAPbI(3) and SnO(2)/MAPbI(3) heterojunction interfaces under high pressure Li, Yuqiang Li, Yuhong Zhang, Qiang Liu, Xiaofeng Li, Yuanjing Xiao, Ningru Ning, Pingfan Wang, Jingjing Zhang, Jianxin Liu, Hongwei RSC Adv Chemistry The electrical transport properties of SnO(2)(TiO(2))/MAPbI(3) (MA = CH(3)NH(3)(+)) heterojunction interfaces are investigated from ambient pressure to 20 GPa, and the transport properties are calculated by physical parameters such as trap energy density, binding energy, and charge transfer driving force and defect. Based on the partial density of states (PDOS) of the SnO(2)/MAPbI(3) heterojunction interface MAI-termination and PbI(2)-termination, greater charge transfer driving force and higher binding energy are observed, obviously showing the SnO(2)-based heterojunction is more stable. The SnO(2)/MAPbI(3) heterojunction interface possesses stronger electrical transport ability and is less prone to capture electrons compared with the TiO(2)/MAPbI(3) heterojunction interface. The differential charge density spectrum shows that the density is lower in the trap energy level of SnO(2)/MAPbI(3), whilst the effect of the charge transfer defect is weaker owing to the trap energy level only existing in SnO(2). The SnO(2)/MAPbI(3) heterostructure interface is less prone to capture electrons. The greater electron concentration difference is attributed to oxygen vacancy (Vo(0)) in the SnO-like environment, resulting in superior electron transport ability compared with the TiO-like environment. The Royal Society of Chemistry 2023-01-23 /pmc/articles/PMC9869466/ /pubmed/36756422 http://dx.doi.org/10.1039/d2ra08143a Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/ |
spellingShingle | Chemistry Li, Yuqiang Li, Yuhong Zhang, Qiang Liu, Xiaofeng Li, Yuanjing Xiao, Ningru Ning, Pingfan Wang, Jingjing Zhang, Jianxin Liu, Hongwei Electrical transport properties of TiO(2)/MAPbI(3) and SnO(2)/MAPbI(3) heterojunction interfaces under high pressure |
title | Electrical transport properties of TiO(2)/MAPbI(3) and SnO(2)/MAPbI(3) heterojunction interfaces under high pressure |
title_full | Electrical transport properties of TiO(2)/MAPbI(3) and SnO(2)/MAPbI(3) heterojunction interfaces under high pressure |
title_fullStr | Electrical transport properties of TiO(2)/MAPbI(3) and SnO(2)/MAPbI(3) heterojunction interfaces under high pressure |
title_full_unstemmed | Electrical transport properties of TiO(2)/MAPbI(3) and SnO(2)/MAPbI(3) heterojunction interfaces under high pressure |
title_short | Electrical transport properties of TiO(2)/MAPbI(3) and SnO(2)/MAPbI(3) heterojunction interfaces under high pressure |
title_sort | electrical transport properties of tio(2)/mapbi(3) and sno(2)/mapbi(3) heterojunction interfaces under high pressure |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9869466/ https://www.ncbi.nlm.nih.gov/pubmed/36756422 http://dx.doi.org/10.1039/d2ra08143a |
work_keys_str_mv | AT liyuqiang electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure AT liyuhong electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure AT zhangqiang electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure AT liuxiaofeng electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure AT liyuanjing electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure AT xiaoningru electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure AT ningpingfan electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure AT wangjingjing electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure AT zhangjianxin electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure AT liuhongwei electricaltransportpropertiesoftio2mapbi3andsno2mapbi3heterojunctioninterfacesunderhighpressure |