Cargando…

Anisotropic electrical resistance in mesoscopic LaAlO(3)/SrTiO(3) devices with individual domain walls

The crystal structure of bulk SrTiO(3)(STO) transitions from cubic to tetragonal at around 105 K. Recent local scanning probe measurements of LaAlO(3)/SrTiO(3) (LAO/STO) interfaces indicated the existence of spatially inhomogeneous electrical current paths and electrostatic potential associated with...

Descripción completa

Detalles Bibliográficos
Autores principales: Goble, Nicholas J., Akrobetu, Richard, Zaid, Hicham, Sucharitakul, Sukrit, Berger, Marie-Hélène, Sehirlioglu, Alp, Gao, Xuan P. A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5353628/
https://www.ncbi.nlm.nih.gov/pubmed/28295058
http://dx.doi.org/10.1038/srep44361
_version_ 1782515152501866496
author Goble, Nicholas J.
Akrobetu, Richard
Zaid, Hicham
Sucharitakul, Sukrit
Berger, Marie-Hélène
Sehirlioglu, Alp
Gao, Xuan P. A.
author_facet Goble, Nicholas J.
Akrobetu, Richard
Zaid, Hicham
Sucharitakul, Sukrit
Berger, Marie-Hélène
Sehirlioglu, Alp
Gao, Xuan P. A.
author_sort Goble, Nicholas J.
collection PubMed
description The crystal structure of bulk SrTiO(3)(STO) transitions from cubic to tetragonal at around 105 K. Recent local scanning probe measurements of LaAlO(3)/SrTiO(3) (LAO/STO) interfaces indicated the existence of spatially inhomogeneous electrical current paths and electrostatic potential associated with the structural domain formation in the tetragonal phase of STO. Here we report a study of temperature dependent electronic transport in combination with the polarized light microscopy of structural domains in mesoscopic LAO/STO devices. By reducing the size of the conductive interface to be comparable to that of a single tetragonal domain of STO, the anisotropy of interfacial electron conduction in relationship to the domain wall and its direction was characterized between T = 10–300 K. It was found that the four-point resistance measured with current parallel to the domain wall is larger than the resistance measured perpendicular to the domain wall. This observation is qualitatively consistent with the current diverting effect from a more conductive domain wall within the sample. Among all the samples studied, the maximum resistance ratio found is at least 10 and could be as large as 10(5) at T = 10 K. This electronic anisotropy may have implications on other oxide hetero-interfaces and the further understanding of electronic/magnetic phenomena found in LAO/STO.
format Online
Article
Text
id pubmed-5353628
institution National Center for Biotechnology Information
language English
publishDate 2017
publisher Nature Publishing Group
record_format MEDLINE/PubMed
spelling pubmed-53536282017-03-20 Anisotropic electrical resistance in mesoscopic LaAlO(3)/SrTiO(3) devices with individual domain walls Goble, Nicholas J. Akrobetu, Richard Zaid, Hicham Sucharitakul, Sukrit Berger, Marie-Hélène Sehirlioglu, Alp Gao, Xuan P. A. Sci Rep Article The crystal structure of bulk SrTiO(3)(STO) transitions from cubic to tetragonal at around 105 K. Recent local scanning probe measurements of LaAlO(3)/SrTiO(3) (LAO/STO) interfaces indicated the existence of spatially inhomogeneous electrical current paths and electrostatic potential associated with the structural domain formation in the tetragonal phase of STO. Here we report a study of temperature dependent electronic transport in combination with the polarized light microscopy of structural domains in mesoscopic LAO/STO devices. By reducing the size of the conductive interface to be comparable to that of a single tetragonal domain of STO, the anisotropy of interfacial electron conduction in relationship to the domain wall and its direction was characterized between T = 10–300 K. It was found that the four-point resistance measured with current parallel to the domain wall is larger than the resistance measured perpendicular to the domain wall. This observation is qualitatively consistent with the current diverting effect from a more conductive domain wall within the sample. Among all the samples studied, the maximum resistance ratio found is at least 10 and could be as large as 10(5) at T = 10 K. This electronic anisotropy may have implications on other oxide hetero-interfaces and the further understanding of electronic/magnetic phenomena found in LAO/STO. Nature Publishing Group 2017-03-15 /pmc/articles/PMC5353628/ /pubmed/28295058 http://dx.doi.org/10.1038/srep44361 Text en Copyright © 2017, The Author(s) http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/
spellingShingle Article
Goble, Nicholas J.
Akrobetu, Richard
Zaid, Hicham
Sucharitakul, Sukrit
Berger, Marie-Hélène
Sehirlioglu, Alp
Gao, Xuan P. A.
Anisotropic electrical resistance in mesoscopic LaAlO(3)/SrTiO(3) devices with individual domain walls
title Anisotropic electrical resistance in mesoscopic LaAlO(3)/SrTiO(3) devices with individual domain walls
title_full Anisotropic electrical resistance in mesoscopic LaAlO(3)/SrTiO(3) devices with individual domain walls
title_fullStr Anisotropic electrical resistance in mesoscopic LaAlO(3)/SrTiO(3) devices with individual domain walls
title_full_unstemmed Anisotropic electrical resistance in mesoscopic LaAlO(3)/SrTiO(3) devices with individual domain walls
title_short Anisotropic electrical resistance in mesoscopic LaAlO(3)/SrTiO(3) devices with individual domain walls
title_sort anisotropic electrical resistance in mesoscopic laalo(3)/srtio(3) devices with individual domain walls
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5353628/
https://www.ncbi.nlm.nih.gov/pubmed/28295058
http://dx.doi.org/10.1038/srep44361
work_keys_str_mv AT goblenicholasj anisotropicelectricalresistanceinmesoscopiclaalo3srtio3deviceswithindividualdomainwalls
AT akrobeturichard anisotropicelectricalresistanceinmesoscopiclaalo3srtio3deviceswithindividualdomainwalls
AT zaidhicham anisotropicelectricalresistanceinmesoscopiclaalo3srtio3deviceswithindividualdomainwalls
AT sucharitakulsukrit anisotropicelectricalresistanceinmesoscopiclaalo3srtio3deviceswithindividualdomainwalls
AT bergermariehelene anisotropicelectricalresistanceinmesoscopiclaalo3srtio3deviceswithindividualdomainwalls
AT sehirlioglualp anisotropicelectricalresistanceinmesoscopiclaalo3srtio3deviceswithindividualdomainwalls
AT gaoxuanpa anisotropicelectricalresistanceinmesoscopiclaalo3srtio3deviceswithindividualdomainwalls