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Critical field of 2H-NbSe(2) down to 50mK

Critical field of 2H-NbSe(2) is determined for the field perpendicular to the conducting planes down to 50 mK, by magnetoresistance measurements. It is the first time that such a measurement is extended below 1 K. Variations are almost linear down to 1 K, with a little upward curvature, and the slop...

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Detalles Bibliográficos
Autores principales: Nader, Adel, Monceau, Pierre
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer International Publishing 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4320156/
https://www.ncbi.nlm.nih.gov/pubmed/25674423
http://dx.doi.org/10.1186/2193-1801-3-16
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author Nader, Adel
Monceau, Pierre
author_facet Nader, Adel
Monceau, Pierre
author_sort Nader, Adel
collection PubMed
description Critical field of 2H-NbSe(2) is determined for the field perpendicular to the conducting planes down to 50 mK, by magnetoresistance measurements. It is the first time that such a measurement is extended below 1 K. Variations are almost linear down to 1 K, with a little upward curvature, and the slope of H(c 2⊥) (T) decreases below 1 K. The reduced critical field extrapolates to 0.9 when the temperature approaches zero, higher than the WHH upper limit of 0.69 conformably with the extension of this model for anisotropic superconductors. Angular dependence of the critical field is also determined at 5.5 K. Variations are the same as expected for a 3D-anisotrpic superconductor and the anisotropy value confirms previous results.
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spelling pubmed-43201562015-02-11 Critical field of 2H-NbSe(2) down to 50mK Nader, Adel Monceau, Pierre Springerplus Short Report Critical field of 2H-NbSe(2) is determined for the field perpendicular to the conducting planes down to 50 mK, by magnetoresistance measurements. It is the first time that such a measurement is extended below 1 K. Variations are almost linear down to 1 K, with a little upward curvature, and the slope of H(c 2⊥) (T) decreases below 1 K. The reduced critical field extrapolates to 0.9 when the temperature approaches zero, higher than the WHH upper limit of 0.69 conformably with the extension of this model for anisotropic superconductors. Angular dependence of the critical field is also determined at 5.5 K. Variations are the same as expected for a 3D-anisotrpic superconductor and the anisotropy value confirms previous results. Springer International Publishing 2014-01-09 /pmc/articles/PMC4320156/ /pubmed/25674423 http://dx.doi.org/10.1186/2193-1801-3-16 Text en © Nader and Monceau; licensee Springer. 2014 This article is published under license to BioMed Central Ltd. 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 Short Report
Nader, Adel
Monceau, Pierre
Critical field of 2H-NbSe(2) down to 50mK
title Critical field of 2H-NbSe(2) down to 50mK
title_full Critical field of 2H-NbSe(2) down to 50mK
title_fullStr Critical field of 2H-NbSe(2) down to 50mK
title_full_unstemmed Critical field of 2H-NbSe(2) down to 50mK
title_short Critical field of 2H-NbSe(2) down to 50mK
title_sort critical field of 2h-nbse(2) down to 50mk
topic Short Report
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4320156/
https://www.ncbi.nlm.nih.gov/pubmed/25674423
http://dx.doi.org/10.1186/2193-1801-3-16
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