Temperature dependent giant resistance anomaly in LaAlO3/SrTiO3 nanostructures

Abstract The resistance of the electron gas (2DEG) at the interface between the two band insulators LaAlO3 (LAO) and SrTiO3 (STO) typically drops monotonically with temperature and R/T curves during cooling and warm-up look identical for large area structures. Here we show that if the LAO/STO is lat...

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Main Authors: M. Z. Minhas, A. Müller, F. Heyroth, H. H. Blaschek, G. Schmidt
Format: Article
Language:English
Published: Nature Publishing Group 2017-07-01
Series:Scientific Reports
Online Access:https://doi.org/10.1038/s41598-017-05331-y
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spelling doaj-8e53c54d9c6a45c6ad6a5ae4aab157b82020-12-08T01:05:45ZengNature Publishing GroupScientific Reports2045-23222017-07-01711910.1038/s41598-017-05331-yTemperature dependent giant resistance anomaly in LaAlO3/SrTiO3 nanostructuresM. Z. Minhas0A. Müller1F. Heyroth2H. H. Blaschek3G. Schmidt4Institut für Physik, Martin-Luther-Universität Halle-WittenbergInstitut für Physik, Martin-Luther-Universität Halle-WittenbergInterdisziplinäres Zentrum für Materialwissenschaften, Martin-Luther-Universität Halle-WittenbergInstitut für Physik, Martin-Luther-Universität Halle-WittenbergInstitut für Physik, Martin-Luther-Universität Halle-WittenbergAbstract The resistance of the electron gas (2DEG) at the interface between the two band insulators LaAlO3 (LAO) and SrTiO3 (STO) typically drops monotonically with temperature and R/T curves during cooling and warm-up look identical for large area structures. Here we show that if the LAO/STO is laterally restricted by nanopatterning the resistance exhibits a temperature anomaly. Warming up nanostructures from low temperatures leads to one or two pronounced resistance peaks between 50 and 100 K not observed for larger dimensions. During cool-down current filaments emerge at the domain walls that form during a structural phase transition of the STO substrate. During warm-up the reverse phase transition can interrupt filaments before the sheet conductivity which dominates at higher temperature is reestablished. Due to the limited number of filaments in a nanostructure this process can result in a complete loss of conductance. As a consequence of these findings the transport physics extracted from experiments in small and large area LAO/STO structures may need to be reconsidered.https://doi.org/10.1038/s41598-017-05331-y
collection DOAJ
language English
format Article
sources DOAJ
author M. Z. Minhas
A. Müller
F. Heyroth
H. H. Blaschek
G. Schmidt
spellingShingle M. Z. Minhas
A. Müller
F. Heyroth
H. H. Blaschek
G. Schmidt
Temperature dependent giant resistance anomaly in LaAlO3/SrTiO3 nanostructures
Scientific Reports
author_facet M. Z. Minhas
A. Müller
F. Heyroth
H. H. Blaschek
G. Schmidt
author_sort M. Z. Minhas
title Temperature dependent giant resistance anomaly in LaAlO3/SrTiO3 nanostructures
title_short Temperature dependent giant resistance anomaly in LaAlO3/SrTiO3 nanostructures
title_full Temperature dependent giant resistance anomaly in LaAlO3/SrTiO3 nanostructures
title_fullStr Temperature dependent giant resistance anomaly in LaAlO3/SrTiO3 nanostructures
title_full_unstemmed Temperature dependent giant resistance anomaly in LaAlO3/SrTiO3 nanostructures
title_sort temperature dependent giant resistance anomaly in laalo3/srtio3 nanostructures
publisher Nature Publishing Group
series Scientific Reports
issn 2045-2322
publishDate 2017-07-01
description Abstract The resistance of the electron gas (2DEG) at the interface between the two band insulators LaAlO3 (LAO) and SrTiO3 (STO) typically drops monotonically with temperature and R/T curves during cooling and warm-up look identical for large area structures. Here we show that if the LAO/STO is laterally restricted by nanopatterning the resistance exhibits a temperature anomaly. Warming up nanostructures from low temperatures leads to one or two pronounced resistance peaks between 50 and 100 K not observed for larger dimensions. During cool-down current filaments emerge at the domain walls that form during a structural phase transition of the STO substrate. During warm-up the reverse phase transition can interrupt filaments before the sheet conductivity which dominates at higher temperature is reestablished. Due to the limited number of filaments in a nanostructure this process can result in a complete loss of conductance. As a consequence of these findings the transport physics extracted from experiments in small and large area LAO/STO structures may need to be reconsidered.
url https://doi.org/10.1038/s41598-017-05331-y
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