Cargando…

Dynamics and mechanism of oxygen annealing in Fe(1+y)Te(0.6)Se(0.4) single crystal

Iron chalcogenide Fe(Te,Se) attracted much attention due to its simple structure, which is favorable for probing the superconducting mechanism. Its less toxic nature compared with iron arsenides is also advantageous for applications of iron-based superconductors. By intercalating spacer layers, supe...

Descripción completa

Detalles Bibliográficos
Autores principales: Sun, Yue, Tsuchiya, Yuji, Taen, Toshihiro, Yamada, Tatsuhiro, Pyon, Sunseng, Sugimoto, Akira, Ekino, Toshikazu, Shi, Zhixiang, Tamegai, Tsuyoshi
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3974131/
https://www.ncbi.nlm.nih.gov/pubmed/24695095
http://dx.doi.org/10.1038/srep04585
_version_ 1782479436670566400
author Sun, Yue
Tsuchiya, Yuji
Taen, Toshihiro
Yamada, Tatsuhiro
Pyon, Sunseng
Sugimoto, Akira
Ekino, Toshikazu
Shi, Zhixiang
Tamegai, Tsuyoshi
author_facet Sun, Yue
Tsuchiya, Yuji
Taen, Toshihiro
Yamada, Tatsuhiro
Pyon, Sunseng
Sugimoto, Akira
Ekino, Toshikazu
Shi, Zhixiang
Tamegai, Tsuyoshi
author_sort Sun, Yue
collection PubMed
description Iron chalcogenide Fe(Te,Se) attracted much attention due to its simple structure, which is favorable for probing the superconducting mechanism. Its less toxic nature compared with iron arsenides is also advantageous for applications of iron-based superconductors. By intercalating spacer layers, superconducting transition temperature has been raised over 40 K. On the other hand, the presence of excess Fe is almost unavoidable in Fe(Te,Se) single crystals, which hinders the appearance of bulk superconductivity and causes strong controversies over its fundamental properties. Here we report a Systematical study of O(2)-annealing dynamics in Fe(1+y)Te(1−x)Se(x) by controlling the amount of O(2), annealing temperature, and time. Bulk superconductivity can be gradually induced by increasing the amount of O(2) and annealing time at suitable temperatures. The optimally annealed crystals can be easily obtained by annealing with ~1.5% molar ratio of oxygen at 400°C for more than 1 hour. Superconductivity was witnessed to evolve mainly from the edge of the crystal to the central part. After the optimal annealing, the complete removal of excess Fe was demonstrated via STM measurements. Some fundamental properties were recharacterized and compared with those of as-grown crystals to discuss the influence of excess Fe.
format Online
Article
Text
id pubmed-3974131
institution National Center for Biotechnology Information
language English
publishDate 2014
publisher Nature Publishing Group
record_format MEDLINE/PubMed
spelling pubmed-39741312014-04-03 Dynamics and mechanism of oxygen annealing in Fe(1+y)Te(0.6)Se(0.4) single crystal Sun, Yue Tsuchiya, Yuji Taen, Toshihiro Yamada, Tatsuhiro Pyon, Sunseng Sugimoto, Akira Ekino, Toshikazu Shi, Zhixiang Tamegai, Tsuyoshi Sci Rep Article Iron chalcogenide Fe(Te,Se) attracted much attention due to its simple structure, which is favorable for probing the superconducting mechanism. Its less toxic nature compared with iron arsenides is also advantageous for applications of iron-based superconductors. By intercalating spacer layers, superconducting transition temperature has been raised over 40 K. On the other hand, the presence of excess Fe is almost unavoidable in Fe(Te,Se) single crystals, which hinders the appearance of bulk superconductivity and causes strong controversies over its fundamental properties. Here we report a Systematical study of O(2)-annealing dynamics in Fe(1+y)Te(1−x)Se(x) by controlling the amount of O(2), annealing temperature, and time. Bulk superconductivity can be gradually induced by increasing the amount of O(2) and annealing time at suitable temperatures. The optimally annealed crystals can be easily obtained by annealing with ~1.5% molar ratio of oxygen at 400°C for more than 1 hour. Superconductivity was witnessed to evolve mainly from the edge of the crystal to the central part. After the optimal annealing, the complete removal of excess Fe was demonstrated via STM measurements. Some fundamental properties were recharacterized and compared with those of as-grown crystals to discuss the influence of excess Fe. Nature Publishing Group 2014-04-03 /pmc/articles/PMC3974131/ /pubmed/24695095 http://dx.doi.org/10.1038/srep04585 Text en Copyright © 2014, Macmillan Publishers Limited. All rights reserved http://creativecommons.org/licenses/by-nc-sa/3.0/ This work is licensed under a Creative Commons Attribution-NonCommercial-ShareAlike 3.0 Unported license. The images in this article are included in the article's Creative Commons license, unless indicated otherwise in the image credit; if the image is not included under the Creative Commons license, users will need to obtain permission from the license holder in order to reproduce the image. To view a copy of this license, visit http://creativecommons.org/licenses/by-nc-sa/3.0/
spellingShingle Article
Sun, Yue
Tsuchiya, Yuji
Taen, Toshihiro
Yamada, Tatsuhiro
Pyon, Sunseng
Sugimoto, Akira
Ekino, Toshikazu
Shi, Zhixiang
Tamegai, Tsuyoshi
Dynamics and mechanism of oxygen annealing in Fe(1+y)Te(0.6)Se(0.4) single crystal
title Dynamics and mechanism of oxygen annealing in Fe(1+y)Te(0.6)Se(0.4) single crystal
title_full Dynamics and mechanism of oxygen annealing in Fe(1+y)Te(0.6)Se(0.4) single crystal
title_fullStr Dynamics and mechanism of oxygen annealing in Fe(1+y)Te(0.6)Se(0.4) single crystal
title_full_unstemmed Dynamics and mechanism of oxygen annealing in Fe(1+y)Te(0.6)Se(0.4) single crystal
title_short Dynamics and mechanism of oxygen annealing in Fe(1+y)Te(0.6)Se(0.4) single crystal
title_sort dynamics and mechanism of oxygen annealing in fe(1+y)te(0.6)se(0.4) single crystal
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3974131/
https://www.ncbi.nlm.nih.gov/pubmed/24695095
http://dx.doi.org/10.1038/srep04585
work_keys_str_mv AT sunyue dynamicsandmechanismofoxygenannealinginfe1yte06se04singlecrystal
AT tsuchiyayuji dynamicsandmechanismofoxygenannealinginfe1yte06se04singlecrystal
AT taentoshihiro dynamicsandmechanismofoxygenannealinginfe1yte06se04singlecrystal
AT yamadatatsuhiro dynamicsandmechanismofoxygenannealinginfe1yte06se04singlecrystal
AT pyonsunseng dynamicsandmechanismofoxygenannealinginfe1yte06se04singlecrystal
AT sugimotoakira dynamicsandmechanismofoxygenannealinginfe1yte06se04singlecrystal
AT ekinotoshikazu dynamicsandmechanismofoxygenannealinginfe1yte06se04singlecrystal
AT shizhixiang dynamicsandmechanismofoxygenannealinginfe1yte06se04singlecrystal
AT tamegaitsuyoshi dynamicsandmechanismofoxygenannealinginfe1yte06se04singlecrystal