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Microstructure and local electrical behavior in [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) (n = 4–8) superlattices

Artificial [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) superlattices (n = 4 and 8) were successfully epitaxially grown on SrTiO(3) substrates by pulsed laser deposition using the in situ high energy electron diffraction reflection diagnostic. The crystallographic relationships between Nd(2)Ti(2)O(7) (NT...

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Autores principales: Carlier, Thomas, Ferri, Anthony, Saitzek, Sébastien, Huvé, Marielle, Bayart, Alexandre, Da Costa, Antonio, Desfeux, Rachel, Tebano, Antonello
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9078952/
https://www.ncbi.nlm.nih.gov/pubmed/35542786
http://dx.doi.org/10.1039/c8ra00824h
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author Carlier, Thomas
Ferri, Anthony
Saitzek, Sébastien
Huvé, Marielle
Bayart, Alexandre
Da Costa, Antonio
Desfeux, Rachel
Tebano, Antonello
author_facet Carlier, Thomas
Ferri, Anthony
Saitzek, Sébastien
Huvé, Marielle
Bayart, Alexandre
Da Costa, Antonio
Desfeux, Rachel
Tebano, Antonello
author_sort Carlier, Thomas
collection PubMed
description Artificial [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) superlattices (n = 4 and 8) were successfully epitaxially grown on SrTiO(3) substrates by pulsed laser deposition using the in situ high energy electron diffraction reflection diagnostic. The crystallographic relationships between Nd(2)Ti(2)O(7) (NTO) and SrTiO(3) (STO) (layers and substrate) were: [100](NTO)//[001](STO), [010](NTO)//[1̄10](STO), and (00l)(NTO)//(110)(STO). Nanoscale current variation was detected on both superlattices, with the (NTO(4)/STO(4))(10) heterostructure showing a higher density. The (NTO(4)/STO(4))(10) sample did not show a piezoelectric response when measured by piezo-force microscopy (PFM), while ambiguous piezoactivity was observed on the (NTO(4)/STO(8))(10) superlattice. Scanning transmission electron microscopy energy dispersive spectroscopy analysis showed the diffusion of Nd(3+) cations on Sr(2+) sites in SrTiO(3) structure into the multilayers, which was more pronounced when the value of n was lower. These particular nanoscale electrical behaviors, evidenced by electrical conducting channels and misleading PFM signals, were mainly attributed to the presence of oxygen vacancies in the SrTiO(3) layers at higher concentrations near the interface and to the mixed valence state of the titanium (Ti(3+)/Ti(4+)). This work showed the strong influence of interface structure on nanoscale electrical phenomena in complex oxide superlattices.
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spelling pubmed-90789522022-05-09 Microstructure and local electrical behavior in [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) (n = 4–8) superlattices Carlier, Thomas Ferri, Anthony Saitzek, Sébastien Huvé, Marielle Bayart, Alexandre Da Costa, Antonio Desfeux, Rachel Tebano, Antonello RSC Adv Chemistry Artificial [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) superlattices (n = 4 and 8) were successfully epitaxially grown on SrTiO(3) substrates by pulsed laser deposition using the in situ high energy electron diffraction reflection diagnostic. The crystallographic relationships between Nd(2)Ti(2)O(7) (NTO) and SrTiO(3) (STO) (layers and substrate) were: [100](NTO)//[001](STO), [010](NTO)//[1̄10](STO), and (00l)(NTO)//(110)(STO). Nanoscale current variation was detected on both superlattices, with the (NTO(4)/STO(4))(10) heterostructure showing a higher density. The (NTO(4)/STO(4))(10) sample did not show a piezoelectric response when measured by piezo-force microscopy (PFM), while ambiguous piezoactivity was observed on the (NTO(4)/STO(8))(10) superlattice. Scanning transmission electron microscopy energy dispersive spectroscopy analysis showed the diffusion of Nd(3+) cations on Sr(2+) sites in SrTiO(3) structure into the multilayers, which was more pronounced when the value of n was lower. These particular nanoscale electrical behaviors, evidenced by electrical conducting channels and misleading PFM signals, were mainly attributed to the presence of oxygen vacancies in the SrTiO(3) layers at higher concentrations near the interface and to the mixed valence state of the titanium (Ti(3+)/Ti(4+)). This work showed the strong influence of interface structure on nanoscale electrical phenomena in complex oxide superlattices. The Royal Society of Chemistry 2018-03-21 /pmc/articles/PMC9078952/ /pubmed/35542786 http://dx.doi.org/10.1039/c8ra00824h Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by/3.0/
spellingShingle Chemistry
Carlier, Thomas
Ferri, Anthony
Saitzek, Sébastien
Huvé, Marielle
Bayart, Alexandre
Da Costa, Antonio
Desfeux, Rachel
Tebano, Antonello
Microstructure and local electrical behavior in [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) (n = 4–8) superlattices
title Microstructure and local electrical behavior in [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) (n = 4–8) superlattices
title_full Microstructure and local electrical behavior in [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) (n = 4–8) superlattices
title_fullStr Microstructure and local electrical behavior in [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) (n = 4–8) superlattices
title_full_unstemmed Microstructure and local electrical behavior in [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) (n = 4–8) superlattices
title_short Microstructure and local electrical behavior in [(Nd(2)Ti(2)O(7))(4)/(SrTiO(3))(n)](10) (n = 4–8) superlattices
title_sort microstructure and local electrical behavior in [(nd(2)ti(2)o(7))(4)/(srtio(3))(n)](10) (n = 4–8) superlattices
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9078952/
https://www.ncbi.nlm.nih.gov/pubmed/35542786
http://dx.doi.org/10.1039/c8ra00824h
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