Cargando…
Two-dimensional polar metals in KNbO(3)/BaTiO(3) superlattices: first-principle calculations
Polar metals, commonly defined by the coexistence of polar structure and metallicity, are thought to be scarce because free carriers eliminate internal dipoles that may arise owing to asymmetric charge distributions. By using first-principle electronic structure calculations, we explored the possibi...
Autores principales: | , , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2019
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9074721/ https://www.ncbi.nlm.nih.gov/pubmed/35528067 http://dx.doi.org/10.1039/c9ra06209b |
_version_ | 1784701532021719040 |
---|---|
author | Li, Gang Huang, Huiyu Peng, Shaoqin Xiong, Ying Xiao, Yongguang Yan, Shaoan Cao, Yanwei Tang, Minghua Li, Zheng |
author_facet | Li, Gang Huang, Huiyu Peng, Shaoqin Xiong, Ying Xiao, Yongguang Yan, Shaoan Cao, Yanwei Tang, Minghua Li, Zheng |
author_sort | Li, Gang |
collection | PubMed |
description | Polar metals, commonly defined by the coexistence of polar structure and metallicity, are thought to be scarce because free carriers eliminate internal dipoles that may arise owing to asymmetric charge distributions. By using first-principle electronic structure calculations, we explored the possibility of producing metallic states in the polar/nonpolar KNbO(3)/BaTiO(3) superlattice (SL) composed of two prototypical ferroelectric materials: BaTiO(3) (BTO) and KNbO(3) (KNO). Two types of polar/nonpolar interfaces, p-type (KO)(−)/(TiO(2))(0) and n-type (NbO(2))(+)/(BaO)(0), which can be constituted into two symmetric NbO(2)/BaO–NbO(2)/BaO (NN-type) and KO/TiO(2)–KO/TiO(2) (PP-type) SL, as well as one asymmetric KO/TiO(2)–NbO(2)/BaO (PN-type) SL. The spatial distribution of ferroelectric distortions and their conductive properties are found to be extraordinarily sensitive to the interfacial configurations. An insulator-to-metal transition is found in each unit cell of the symmetric interfacial SL models: one exhibiting quasi-two-dimensional n-type conductivity for NN-type SL, while the other being quasi-two-dimensional p-type conductivity for PP-type SL. The anisotropic coexistence of in-plane orientation of free carriers and out-of-plane orientation of ferroelectric polarization in KNO/BTO SL indicates that in-plane free carriers can not eliminate the out-of-plane dipoles. Our results provide a road map to create two-dimensional polar metals in insulating perovskite oxide SL, which is expected to promote applications of new quantum devices. |
format | Online Article Text |
id | pubmed-9074721 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | The Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
spelling | pubmed-90747212022-05-06 Two-dimensional polar metals in KNbO(3)/BaTiO(3) superlattices: first-principle calculations Li, Gang Huang, Huiyu Peng, Shaoqin Xiong, Ying Xiao, Yongguang Yan, Shaoan Cao, Yanwei Tang, Minghua Li, Zheng RSC Adv Chemistry Polar metals, commonly defined by the coexistence of polar structure and metallicity, are thought to be scarce because free carriers eliminate internal dipoles that may arise owing to asymmetric charge distributions. By using first-principle electronic structure calculations, we explored the possibility of producing metallic states in the polar/nonpolar KNbO(3)/BaTiO(3) superlattice (SL) composed of two prototypical ferroelectric materials: BaTiO(3) (BTO) and KNbO(3) (KNO). Two types of polar/nonpolar interfaces, p-type (KO)(−)/(TiO(2))(0) and n-type (NbO(2))(+)/(BaO)(0), which can be constituted into two symmetric NbO(2)/BaO–NbO(2)/BaO (NN-type) and KO/TiO(2)–KO/TiO(2) (PP-type) SL, as well as one asymmetric KO/TiO(2)–NbO(2)/BaO (PN-type) SL. The spatial distribution of ferroelectric distortions and their conductive properties are found to be extraordinarily sensitive to the interfacial configurations. An insulator-to-metal transition is found in each unit cell of the symmetric interfacial SL models: one exhibiting quasi-two-dimensional n-type conductivity for NN-type SL, while the other being quasi-two-dimensional p-type conductivity for PP-type SL. The anisotropic coexistence of in-plane orientation of free carriers and out-of-plane orientation of ferroelectric polarization in KNO/BTO SL indicates that in-plane free carriers can not eliminate the out-of-plane dipoles. Our results provide a road map to create two-dimensional polar metals in insulating perovskite oxide SL, which is expected to promote applications of new quantum devices. The Royal Society of Chemistry 2019-11-01 /pmc/articles/PMC9074721/ /pubmed/35528067 http://dx.doi.org/10.1039/c9ra06209b Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/ |
spellingShingle | Chemistry Li, Gang Huang, Huiyu Peng, Shaoqin Xiong, Ying Xiao, Yongguang Yan, Shaoan Cao, Yanwei Tang, Minghua Li, Zheng Two-dimensional polar metals in KNbO(3)/BaTiO(3) superlattices: first-principle calculations |
title | Two-dimensional polar metals in KNbO(3)/BaTiO(3) superlattices: first-principle calculations |
title_full | Two-dimensional polar metals in KNbO(3)/BaTiO(3) superlattices: first-principle calculations |
title_fullStr | Two-dimensional polar metals in KNbO(3)/BaTiO(3) superlattices: first-principle calculations |
title_full_unstemmed | Two-dimensional polar metals in KNbO(3)/BaTiO(3) superlattices: first-principle calculations |
title_short | Two-dimensional polar metals in KNbO(3)/BaTiO(3) superlattices: first-principle calculations |
title_sort | two-dimensional polar metals in knbo(3)/batio(3) superlattices: first-principle calculations |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9074721/ https://www.ncbi.nlm.nih.gov/pubmed/35528067 http://dx.doi.org/10.1039/c9ra06209b |
work_keys_str_mv | AT ligang twodimensionalpolarmetalsinknbo3batio3superlatticesfirstprinciplecalculations AT huanghuiyu twodimensionalpolarmetalsinknbo3batio3superlatticesfirstprinciplecalculations AT pengshaoqin twodimensionalpolarmetalsinknbo3batio3superlatticesfirstprinciplecalculations AT xiongying twodimensionalpolarmetalsinknbo3batio3superlatticesfirstprinciplecalculations AT xiaoyongguang twodimensionalpolarmetalsinknbo3batio3superlatticesfirstprinciplecalculations AT yanshaoan twodimensionalpolarmetalsinknbo3batio3superlatticesfirstprinciplecalculations AT caoyanwei twodimensionalpolarmetalsinknbo3batio3superlatticesfirstprinciplecalculations AT tangminghua twodimensionalpolarmetalsinknbo3batio3superlatticesfirstprinciplecalculations AT lizheng twodimensionalpolarmetalsinknbo3batio3superlatticesfirstprinciplecalculations |