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Influence of the Template Layer on the Structure and Ferroelectric Properties of PbZr(0.52)Ti(0.48)O(3) Films

[Image: see text] The microstructure of the PbZr(0.52)Ti(0.48)O(3) (PZT) films is known to influence the ferroelectric properties, but so far mainly the effect of the deposition conditions of the PZT has been investigated. To our knowledge, the influence of the underlying electrode layer and the mec...

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Autores principales: Lucke, Philip, Nematollahi, Mohammadreza, Bayraktar, Muharrem, Yakshin, Andrey E., ten Elshof, Johan E., Bijkerk, Fred
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9260783/
https://www.ncbi.nlm.nih.gov/pubmed/35811867
http://dx.doi.org/10.1021/acsomega.2c00815
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author Lucke, Philip
Nematollahi, Mohammadreza
Bayraktar, Muharrem
Yakshin, Andrey E.
ten Elshof, Johan E.
Bijkerk, Fred
author_facet Lucke, Philip
Nematollahi, Mohammadreza
Bayraktar, Muharrem
Yakshin, Andrey E.
ten Elshof, Johan E.
Bijkerk, Fred
author_sort Lucke, Philip
collection PubMed
description [Image: see text] The microstructure of the PbZr(0.52)Ti(0.48)O(3) (PZT) films is known to influence the ferroelectric properties, but so far mainly the effect of the deposition conditions of the PZT has been investigated. To our knowledge, the influence of the underlying electrode layer and the mechanisms leading to changes in the PZT microstructure have not been explored. Using LaNiO(3) (LNO) as the bottom electrode material, we investigated the evolution of the PZT microstructure and ferroelectric properties for changing LNO pulsed-laser deposition conditions. The explored deposition conditions were the O(2) pressure, total pressure, and thickness of the electrode layer. Increasing both the O(2) pressure and the thickness of the electrode layer changes the growth of PZT from a smooth, dense film to a rough, columnar film. We explain the origin of the change in PZT microstructure as the increased roughness of the electrode layer in relaxing the misfit strain. The strain relaxation mechanism is evidenced by the increase in the crystal phase with bulk LNO unit cell dimensions in comparison to the crystal phase with substrate-clamped unit cell dimensions. We explain the change from a dense to a columnar microstructure as a result of the change in the growth mode from Frank–van der Merwe to Stranski–Krastanov. The ferroelectric properties of the columnar films are improved compared to those of the smooth, dense films. The ability to tune the ferroelectric properties with the microstructure is primarily relevant for ferroelectric applications such as actuators and systems for energy harvesting and storage.
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spelling pubmed-92607832022-07-08 Influence of the Template Layer on the Structure and Ferroelectric Properties of PbZr(0.52)Ti(0.48)O(3) Films Lucke, Philip Nematollahi, Mohammadreza Bayraktar, Muharrem Yakshin, Andrey E. ten Elshof, Johan E. Bijkerk, Fred ACS Omega [Image: see text] The microstructure of the PbZr(0.52)Ti(0.48)O(3) (PZT) films is known to influence the ferroelectric properties, but so far mainly the effect of the deposition conditions of the PZT has been investigated. To our knowledge, the influence of the underlying electrode layer and the mechanisms leading to changes in the PZT microstructure have not been explored. Using LaNiO(3) (LNO) as the bottom electrode material, we investigated the evolution of the PZT microstructure and ferroelectric properties for changing LNO pulsed-laser deposition conditions. The explored deposition conditions were the O(2) pressure, total pressure, and thickness of the electrode layer. Increasing both the O(2) pressure and the thickness of the electrode layer changes the growth of PZT from a smooth, dense film to a rough, columnar film. We explain the origin of the change in PZT microstructure as the increased roughness of the electrode layer in relaxing the misfit strain. The strain relaxation mechanism is evidenced by the increase in the crystal phase with bulk LNO unit cell dimensions in comparison to the crystal phase with substrate-clamped unit cell dimensions. We explain the change from a dense to a columnar microstructure as a result of the change in the growth mode from Frank–van der Merwe to Stranski–Krastanov. The ferroelectric properties of the columnar films are improved compared to those of the smooth, dense films. The ability to tune the ferroelectric properties with the microstructure is primarily relevant for ferroelectric applications such as actuators and systems for energy harvesting and storage. American Chemical Society 2022-06-17 /pmc/articles/PMC9260783/ /pubmed/35811867 http://dx.doi.org/10.1021/acsomega.2c00815 Text en © 2022 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by-nc-nd/4.0/Permits non-commercial access and re-use, provided that author attribution and integrity are maintained; but does not permit creation of adaptations or other derivative works (https://creativecommons.org/licenses/by-nc-nd/4.0/).
spellingShingle Lucke, Philip
Nematollahi, Mohammadreza
Bayraktar, Muharrem
Yakshin, Andrey E.
ten Elshof, Johan E.
Bijkerk, Fred
Influence of the Template Layer on the Structure and Ferroelectric Properties of PbZr(0.52)Ti(0.48)O(3) Films
title Influence of the Template Layer on the Structure and Ferroelectric Properties of PbZr(0.52)Ti(0.48)O(3) Films
title_full Influence of the Template Layer on the Structure and Ferroelectric Properties of PbZr(0.52)Ti(0.48)O(3) Films
title_fullStr Influence of the Template Layer on the Structure and Ferroelectric Properties of PbZr(0.52)Ti(0.48)O(3) Films
title_full_unstemmed Influence of the Template Layer on the Structure and Ferroelectric Properties of PbZr(0.52)Ti(0.48)O(3) Films
title_short Influence of the Template Layer on the Structure and Ferroelectric Properties of PbZr(0.52)Ti(0.48)O(3) Films
title_sort influence of the template layer on the structure and ferroelectric properties of pbzr(0.52)ti(0.48)o(3) films
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9260783/
https://www.ncbi.nlm.nih.gov/pubmed/35811867
http://dx.doi.org/10.1021/acsomega.2c00815
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