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High field superconducting properties of Ba(Fe(1−x)Co(x))(2)As(2) thin films

In general, the critical current density, J(c), of type II superconductors and its anisotropy with respect to magnetic field orientation is determined by intrinsic and extrinsic properties. The Fe-based superconductors of the ‘122’ family with their moderate electronic anisotropies and high yet acce...

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Autores principales: Hänisch, Jens, Iida, Kazumasa, Kurth, Fritz, Reich, Elke, Tarantini, Chiara, Jaroszynski, Jan, Förster, Tobias, Fuchs, Günther, Hühne, Ruben, Grinenko, Vadim, Schultz, Ludwig, Holzapfel, Bernhard
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4661601/
https://www.ncbi.nlm.nih.gov/pubmed/26612567
http://dx.doi.org/10.1038/srep17363
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author Hänisch, Jens
Iida, Kazumasa
Kurth, Fritz
Reich, Elke
Tarantini, Chiara
Jaroszynski, Jan
Förster, Tobias
Fuchs, Günther
Hühne, Ruben
Grinenko, Vadim
Schultz, Ludwig
Holzapfel, Bernhard
author_facet Hänisch, Jens
Iida, Kazumasa
Kurth, Fritz
Reich, Elke
Tarantini, Chiara
Jaroszynski, Jan
Förster, Tobias
Fuchs, Günther
Hühne, Ruben
Grinenko, Vadim
Schultz, Ludwig
Holzapfel, Bernhard
author_sort Hänisch, Jens
collection PubMed
description In general, the critical current density, J(c), of type II superconductors and its anisotropy with respect to magnetic field orientation is determined by intrinsic and extrinsic properties. The Fe-based superconductors of the ‘122’ family with their moderate electronic anisotropies and high yet accessible critical fields (H(c2) and H(irr)) are a good model system to study this interplay. In this paper, we explore the vortex matter of optimally Co-doped BaFe(2)As(2) thin films with extended planar and c-axis correlated defects. The temperature and angular dependence of the upper critical field is well explained by a two-band model in the clean limit. The dirty band scenario, however, cannot be ruled out completely. Above the irreversibility field, the flux motion is thermally activated, where the activation energy U(0) is going to zero at the extrapolated zero-kelvin H(irr) value. The anisotropy of the critical current density J(c) is both influenced by the H(c2) anisotropy (and therefore by multi-band effects) as well as the extended planar and columnar defects present in the sample.
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spelling pubmed-46616012015-12-01 High field superconducting properties of Ba(Fe(1−x)Co(x))(2)As(2) thin films Hänisch, Jens Iida, Kazumasa Kurth, Fritz Reich, Elke Tarantini, Chiara Jaroszynski, Jan Förster, Tobias Fuchs, Günther Hühne, Ruben Grinenko, Vadim Schultz, Ludwig Holzapfel, Bernhard Sci Rep Article In general, the critical current density, J(c), of type II superconductors and its anisotropy with respect to magnetic field orientation is determined by intrinsic and extrinsic properties. The Fe-based superconductors of the ‘122’ family with their moderate electronic anisotropies and high yet accessible critical fields (H(c2) and H(irr)) are a good model system to study this interplay. In this paper, we explore the vortex matter of optimally Co-doped BaFe(2)As(2) thin films with extended planar and c-axis correlated defects. The temperature and angular dependence of the upper critical field is well explained by a two-band model in the clean limit. The dirty band scenario, however, cannot be ruled out completely. Above the irreversibility field, the flux motion is thermally activated, where the activation energy U(0) is going to zero at the extrapolated zero-kelvin H(irr) value. The anisotropy of the critical current density J(c) is both influenced by the H(c2) anisotropy (and therefore by multi-band effects) as well as the extended planar and columnar defects present in the sample. Nature Publishing Group 2015-11-27 /pmc/articles/PMC4661601/ /pubmed/26612567 http://dx.doi.org/10.1038/srep17363 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
Hänisch, Jens
Iida, Kazumasa
Kurth, Fritz
Reich, Elke
Tarantini, Chiara
Jaroszynski, Jan
Förster, Tobias
Fuchs, Günther
Hühne, Ruben
Grinenko, Vadim
Schultz, Ludwig
Holzapfel, Bernhard
High field superconducting properties of Ba(Fe(1−x)Co(x))(2)As(2) thin films
title High field superconducting properties of Ba(Fe(1−x)Co(x))(2)As(2) thin films
title_full High field superconducting properties of Ba(Fe(1−x)Co(x))(2)As(2) thin films
title_fullStr High field superconducting properties of Ba(Fe(1−x)Co(x))(2)As(2) thin films
title_full_unstemmed High field superconducting properties of Ba(Fe(1−x)Co(x))(2)As(2) thin films
title_short High field superconducting properties of Ba(Fe(1−x)Co(x))(2)As(2) thin films
title_sort high field superconducting properties of ba(fe(1−x)co(x))(2)as(2) thin films
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4661601/
https://www.ncbi.nlm.nih.gov/pubmed/26612567
http://dx.doi.org/10.1038/srep17363
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