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Dependencies of microstructure and stress on the thickness of GdBa(2)Cu(3)O(7 − δ) thin films fabricated by RF sputtering

GdBa(2)Cu(3)O(7 − δ) (GdBCO) films with different thicknesses from 200 to 2,100 nm are deposited on CeO(2)/yttria-stabilized zirconia (YSZ)/CeO(2)-buffered Ni-W substrates by radio-frequency magnetron sputtering. Both the X-ray diffraction and scanning electron microscopy analyses reveal that the a-...

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Detalles Bibliográficos
Autores principales: Wang, Ying, Xu, Da, Li, Yijie, Liu, Linfei
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer 2013
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3716989/
https://www.ncbi.nlm.nih.gov/pubmed/23816137
http://dx.doi.org/10.1186/1556-276X-8-304
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author Wang, Ying
Xu, Da
Li, Yijie
Liu, Linfei
author_facet Wang, Ying
Xu, Da
Li, Yijie
Liu, Linfei
author_sort Wang, Ying
collection PubMed
description GdBa(2)Cu(3)O(7 − δ) (GdBCO) films with different thicknesses from 200 to 2,100 nm are deposited on CeO(2)/yttria-stabilized zirconia (YSZ)/CeO(2)-buffered Ni-W substrates by radio-frequency magnetron sputtering. Both the X-ray diffraction and scanning electron microscopy analyses reveal that the a-axis grains appear at the upper layers of the films when the thickness reaches to 1,030 nm. The X-ray photoelectron spectroscopy measurement implies that the oxygen content is insufficient in upper layers beyond 1,030 nm for a thicker film. The Williamson-Hall method is used to observe the variation of film stress with increasing thickness of our films. It is found that the highest residual stresses exist in the thinnest film, while the lowest residual stresses exist in the 1,030-nm-thick film. With further increasing film thickness, the film residual stresses increase again. However, the critical current (I(c)) of the GdBCO film first shows a nearly linear increase and then shows a more slowly enhancing to a final stagnation as film thickness increases from 200 to 1,030 nm and then to 2,100 nm. It is concluded that the roughness and stress are not the main reasons which cause the slow or no increase in I(c). Also, the thickness dependency of GdBa(2)Cu(3)O(7 − δ) films on the I(c) is attributed to three main factors: a-axis grains, gaps between a-axis grains, and oxygen deficiency for the upper layers of a thick film.
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spelling pubmed-37169892013-07-22 Dependencies of microstructure and stress on the thickness of GdBa(2)Cu(3)O(7 − δ) thin films fabricated by RF sputtering Wang, Ying Xu, Da Li, Yijie Liu, Linfei Nanoscale Res Lett Nano Express GdBa(2)Cu(3)O(7 − δ) (GdBCO) films with different thicknesses from 200 to 2,100 nm are deposited on CeO(2)/yttria-stabilized zirconia (YSZ)/CeO(2)-buffered Ni-W substrates by radio-frequency magnetron sputtering. Both the X-ray diffraction and scanning electron microscopy analyses reveal that the a-axis grains appear at the upper layers of the films when the thickness reaches to 1,030 nm. The X-ray photoelectron spectroscopy measurement implies that the oxygen content is insufficient in upper layers beyond 1,030 nm for a thicker film. The Williamson-Hall method is used to observe the variation of film stress with increasing thickness of our films. It is found that the highest residual stresses exist in the thinnest film, while the lowest residual stresses exist in the 1,030-nm-thick film. With further increasing film thickness, the film residual stresses increase again. However, the critical current (I(c)) of the GdBCO film first shows a nearly linear increase and then shows a more slowly enhancing to a final stagnation as film thickness increases from 200 to 1,030 nm and then to 2,100 nm. It is concluded that the roughness and stress are not the main reasons which cause the slow or no increase in I(c). Also, the thickness dependency of GdBa(2)Cu(3)O(7 − δ) films on the I(c) is attributed to three main factors: a-axis grains, gaps between a-axis grains, and oxygen deficiency for the upper layers of a thick film. Springer 2013-07-01 /pmc/articles/PMC3716989/ /pubmed/23816137 http://dx.doi.org/10.1186/1556-276X-8-304 Text en Copyright ©2013 Wang et al.; licensee Springer. http://creativecommons.org/licenses/by/2.0 This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
spellingShingle Nano Express
Wang, Ying
Xu, Da
Li, Yijie
Liu, Linfei
Dependencies of microstructure and stress on the thickness of GdBa(2)Cu(3)O(7 − δ) thin films fabricated by RF sputtering
title Dependencies of microstructure and stress on the thickness of GdBa(2)Cu(3)O(7 − δ) thin films fabricated by RF sputtering
title_full Dependencies of microstructure and stress on the thickness of GdBa(2)Cu(3)O(7 − δ) thin films fabricated by RF sputtering
title_fullStr Dependencies of microstructure and stress on the thickness of GdBa(2)Cu(3)O(7 − δ) thin films fabricated by RF sputtering
title_full_unstemmed Dependencies of microstructure and stress on the thickness of GdBa(2)Cu(3)O(7 − δ) thin films fabricated by RF sputtering
title_short Dependencies of microstructure and stress on the thickness of GdBa(2)Cu(3)O(7 − δ) thin films fabricated by RF sputtering
title_sort dependencies of microstructure and stress on the thickness of gdba(2)cu(3)o(7 − δ) thin films fabricated by rf sputtering
topic Nano Express
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3716989/
https://www.ncbi.nlm.nih.gov/pubmed/23816137
http://dx.doi.org/10.1186/1556-276X-8-304
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