Cargando…
Anisotropic two-dimensional electron gas at the LaAlO(3)/SrTiO(3) (110) interface
The observation of a high-mobility two-dimensional electron gas between two insulating complex oxides, especially LaAlO(3)/SrTiO(3), has enhanced the potential of oxides for electronics. The occurrence of this conductivity is believed to be driven by polarization discontinuity, leading to an electro...
Autores principales: | , , , , , , , , , , , , , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Pub. Group
2013
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3674248/ https://www.ncbi.nlm.nih.gov/pubmed/23673623 http://dx.doi.org/10.1038/ncomms2804 |
_version_ | 1782272332897714176 |
---|---|
author | Annadi, A. Zhang, Q. Renshaw Wang, X. Tuzla, N. Gopinadhan, K. Lü, W. M. Roy Barman, A. Liu, Z. Q. Srivastava, A. Saha, S. Zhao, Y. L. Zeng, S. W. Dhar, S. Olsson, E. Gu, B. Yunoki, S. Maekawa, S. Hilgenkamp, H. Venkatesan, T. Ariando |
author_facet | Annadi, A. Zhang, Q. Renshaw Wang, X. Tuzla, N. Gopinadhan, K. Lü, W. M. Roy Barman, A. Liu, Z. Q. Srivastava, A. Saha, S. Zhao, Y. L. Zeng, S. W. Dhar, S. Olsson, E. Gu, B. Yunoki, S. Maekawa, S. Hilgenkamp, H. Venkatesan, T. Ariando |
author_sort | Annadi, A. |
collection | PubMed |
description | The observation of a high-mobility two-dimensional electron gas between two insulating complex oxides, especially LaAlO(3)/SrTiO(3), has enhanced the potential of oxides for electronics. The occurrence of this conductivity is believed to be driven by polarization discontinuity, leading to an electronic reconstruction. In this scenario, the crystal orientation has an important role and no conductivity would be expected, for example, for the interface between LaAlO(3) and (110)-oriented SrTiO(3), which should not have a polarization discontinuity. Here we report the observation of unexpected conductivity at the LaAlO(3)/SrTiO(3) interface prepared on (110)-oriented SrTiO(3), with a LaAlO(3)-layer thickness-dependent metal-insulator transition. Density functional theory calculation reveals that electronic reconstruction, and thus conductivity, is still possible at this (110) interface by considering the energetically favourable (110) interface structure, that is, buckled TiO(2)/LaO, in which the polarization discontinuity is still present. The conductivity was further found to be strongly anisotropic along the different crystallographic directions with potential for anisotropic superconductivity and magnetism, leading to possible new physics and applications. |
format | Online Article Text |
id | pubmed-3674248 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2013 |
publisher | Nature Pub. Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-36742482013-06-06 Anisotropic two-dimensional electron gas at the LaAlO(3)/SrTiO(3) (110) interface Annadi, A. Zhang, Q. Renshaw Wang, X. Tuzla, N. Gopinadhan, K. Lü, W. M. Roy Barman, A. Liu, Z. Q. Srivastava, A. Saha, S. Zhao, Y. L. Zeng, S. W. Dhar, S. Olsson, E. Gu, B. Yunoki, S. Maekawa, S. Hilgenkamp, H. Venkatesan, T. Ariando Nat Commun Article The observation of a high-mobility two-dimensional electron gas between two insulating complex oxides, especially LaAlO(3)/SrTiO(3), has enhanced the potential of oxides for electronics. The occurrence of this conductivity is believed to be driven by polarization discontinuity, leading to an electronic reconstruction. In this scenario, the crystal orientation has an important role and no conductivity would be expected, for example, for the interface between LaAlO(3) and (110)-oriented SrTiO(3), which should not have a polarization discontinuity. Here we report the observation of unexpected conductivity at the LaAlO(3)/SrTiO(3) interface prepared on (110)-oriented SrTiO(3), with a LaAlO(3)-layer thickness-dependent metal-insulator transition. Density functional theory calculation reveals that electronic reconstruction, and thus conductivity, is still possible at this (110) interface by considering the energetically favourable (110) interface structure, that is, buckled TiO(2)/LaO, in which the polarization discontinuity is still present. The conductivity was further found to be strongly anisotropic along the different crystallographic directions with potential for anisotropic superconductivity and magnetism, leading to possible new physics and applications. Nature Pub. Group 2013-05-14 /pmc/articles/PMC3674248/ /pubmed/23673623 http://dx.doi.org/10.1038/ncomms2804 Text en Copyright © 2013, Nature Publishing Group, a division of Macmillan Publishers Limited. All Rights Reserved. http://creativecommons.org/licenses/by-nc-nd/3.0/ This work is licensed under a Creative Commons Attribution-NonCommercial-NoDerivs 3.0 Unported License. To view a copy of this license, visit http://creativecommons.org/licenses/by-nc-nd/3.0/ |
spellingShingle | Article Annadi, A. Zhang, Q. Renshaw Wang, X. Tuzla, N. Gopinadhan, K. Lü, W. M. Roy Barman, A. Liu, Z. Q. Srivastava, A. Saha, S. Zhao, Y. L. Zeng, S. W. Dhar, S. Olsson, E. Gu, B. Yunoki, S. Maekawa, S. Hilgenkamp, H. Venkatesan, T. Ariando Anisotropic two-dimensional electron gas at the LaAlO(3)/SrTiO(3) (110) interface |
title | Anisotropic two-dimensional electron gas at the LaAlO(3)/SrTiO(3) (110) interface |
title_full | Anisotropic two-dimensional electron gas at the LaAlO(3)/SrTiO(3) (110) interface |
title_fullStr | Anisotropic two-dimensional electron gas at the LaAlO(3)/SrTiO(3) (110) interface |
title_full_unstemmed | Anisotropic two-dimensional electron gas at the LaAlO(3)/SrTiO(3) (110) interface |
title_short | Anisotropic two-dimensional electron gas at the LaAlO(3)/SrTiO(3) (110) interface |
title_sort | anisotropic two-dimensional electron gas at the laalo(3)/srtio(3) (110) interface |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3674248/ https://www.ncbi.nlm.nih.gov/pubmed/23673623 http://dx.doi.org/10.1038/ncomms2804 |
work_keys_str_mv | AT annadia anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT zhangq anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT renshawwangx anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT tuzlan anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT gopinadhank anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT luwm anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT roybarmana anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT liuzq anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT srivastavaa anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT sahas anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT zhaoyl anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT zengsw anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT dhars anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT olssone anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT gub anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT yunokis anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT maekawas anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT hilgenkamph anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT venkatesant anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface AT ariando anisotropictwodimensionalelectrongasatthelaalo3srtio3110interface |