Cargando…

Universal electronic structure of polar oxide hetero-interfaces

The electronic properties of NdGaO3/SrTiO3, LaGaO3/SrTiO3, and LaAlO3/SrTiO3 interfaces, all showing an insulator-to-metal transition as a function of the overlayer-thickness, are addressed in a comparative study based on x-ray absorption, x-ray photoemission and resonant photoemission spectroscopy....

Descripción completa

Detalles Bibliográficos
Autores principales: Treske, Uwe, Heming, Nadine, Knupfer, Martin, Büchner, Bernd, Gennaro, Emiliano Di, Khare, Amit, Di Uccio, Umberto Scotti, Granozio, Fabio Miletto, Krause, Stefan, Koitzsch, Andreas
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4585978/
https://www.ncbi.nlm.nih.gov/pubmed/26411304
http://dx.doi.org/10.1038/srep14506
_version_ 1782392318269063168
author Treske, Uwe
Heming, Nadine
Knupfer, Martin
Büchner, Bernd
Gennaro, Emiliano Di
Khare, Amit
Di Uccio, Umberto Scotti
Granozio, Fabio Miletto
Krause, Stefan
Koitzsch, Andreas
author_facet Treske, Uwe
Heming, Nadine
Knupfer, Martin
Büchner, Bernd
Gennaro, Emiliano Di
Khare, Amit
Di Uccio, Umberto Scotti
Granozio, Fabio Miletto
Krause, Stefan
Koitzsch, Andreas
author_sort Treske, Uwe
collection PubMed
description The electronic properties of NdGaO3/SrTiO3, LaGaO3/SrTiO3, and LaAlO3/SrTiO3 interfaces, all showing an insulator-to-metal transition as a function of the overlayer-thickness, are addressed in a comparative study based on x-ray absorption, x-ray photoemission and resonant photoemission spectroscopy. The nature of the charge carriers, their concentration and spatial distribution as well as the interface band alignments and the overall interface band diagrams are studied and quantitatively evaluated. The behavior of the three analyzed heterostructures is found to be remarkably similar. The valence band edge of all the three overlayers aligns to that of bulk SrTiO3. The near-interface SrTiO3 layer is affected, at increasing overlayer thickness, by the building-up of a confining potential. This potential bends both the valence and the conduction band downwards. The latter one crossing the Fermi energy in the proximity of the interface and determines the formation of an interfacial band offset growing as a function of thickness. Quite remarkably, but in agreement with previous reports for LaAlO3/SrTiO3, no electric field is detected inside any of the polar overlayers. The essential phenomenology emerging from our findings is discussed on the base of different alternative scenarios regarding the origin of interface carriers and their interaction with an intense photon beam.
format Online
Article
Text
id pubmed-4585978
institution National Center for Biotechnology Information
language English
publishDate 2015
publisher Nature Publishing Group
record_format MEDLINE/PubMed
spelling pubmed-45859782015-09-30 Universal electronic structure of polar oxide hetero-interfaces Treske, Uwe Heming, Nadine Knupfer, Martin Büchner, Bernd Gennaro, Emiliano Di Khare, Amit Di Uccio, Umberto Scotti Granozio, Fabio Miletto Krause, Stefan Koitzsch, Andreas Sci Rep Article The electronic properties of NdGaO3/SrTiO3, LaGaO3/SrTiO3, and LaAlO3/SrTiO3 interfaces, all showing an insulator-to-metal transition as a function of the overlayer-thickness, are addressed in a comparative study based on x-ray absorption, x-ray photoemission and resonant photoemission spectroscopy. The nature of the charge carriers, their concentration and spatial distribution as well as the interface band alignments and the overall interface band diagrams are studied and quantitatively evaluated. The behavior of the three analyzed heterostructures is found to be remarkably similar. The valence band edge of all the three overlayers aligns to that of bulk SrTiO3. The near-interface SrTiO3 layer is affected, at increasing overlayer thickness, by the building-up of a confining potential. This potential bends both the valence and the conduction band downwards. The latter one crossing the Fermi energy in the proximity of the interface and determines the formation of an interfacial band offset growing as a function of thickness. Quite remarkably, but in agreement with previous reports for LaAlO3/SrTiO3, no electric field is detected inside any of the polar overlayers. The essential phenomenology emerging from our findings is discussed on the base of different alternative scenarios regarding the origin of interface carriers and their interaction with an intense photon beam. Nature Publishing Group 2015-09-28 /pmc/articles/PMC4585978/ /pubmed/26411304 http://dx.doi.org/10.1038/srep14506 Text en Copyright © 2015, Macmillan Publishers Limited 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
Treske, Uwe
Heming, Nadine
Knupfer, Martin
Büchner, Bernd
Gennaro, Emiliano Di
Khare, Amit
Di Uccio, Umberto Scotti
Granozio, Fabio Miletto
Krause, Stefan
Koitzsch, Andreas
Universal electronic structure of polar oxide hetero-interfaces
title Universal electronic structure of polar oxide hetero-interfaces
title_full Universal electronic structure of polar oxide hetero-interfaces
title_fullStr Universal electronic structure of polar oxide hetero-interfaces
title_full_unstemmed Universal electronic structure of polar oxide hetero-interfaces
title_short Universal electronic structure of polar oxide hetero-interfaces
title_sort universal electronic structure of polar oxide hetero-interfaces
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4585978/
https://www.ncbi.nlm.nih.gov/pubmed/26411304
http://dx.doi.org/10.1038/srep14506
work_keys_str_mv AT treskeuwe universalelectronicstructureofpolaroxideheterointerfaces
AT hemingnadine universalelectronicstructureofpolaroxideheterointerfaces
AT knupfermartin universalelectronicstructureofpolaroxideheterointerfaces
AT buchnerbernd universalelectronicstructureofpolaroxideheterointerfaces
AT gennaroemilianodi universalelectronicstructureofpolaroxideheterointerfaces
AT khareamit universalelectronicstructureofpolaroxideheterointerfaces
AT diuccioumbertoscotti universalelectronicstructureofpolaroxideheterointerfaces
AT granoziofabiomiletto universalelectronicstructureofpolaroxideheterointerfaces
AT krausestefan universalelectronicstructureofpolaroxideheterointerfaces
AT koitzschandreas universalelectronicstructureofpolaroxideheterointerfaces