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Pressure effect on iron-based superconductor LaFeAsO(1−x)H(x): Peculiar response of 1111-type structure

A systematic study of the crystal structure of a layered iron oxypnictide LaFeAsO(1−x)H(x) as a function of pressure was performed using synchrotron X-ray diffraction. This compound exhibits a unique phase diagram of two superconducting phases and two parent phases. We established that the As–Fe–As...

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Autores principales: Kobayashi, Kensuke, Yamaura, Jun-ichi, Iimura, Soshi, Maki, Sachiko, Sagayama, Hajime, Kumai, Reiji, Murakami, Youichi, Takahashi, Hiroki, Matsuishi, Satoru, Hosono, Hideo
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5177881/
https://www.ncbi.nlm.nih.gov/pubmed/28004768
http://dx.doi.org/10.1038/srep39646
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author Kobayashi, Kensuke
Yamaura, Jun-ichi
Iimura, Soshi
Maki, Sachiko
Sagayama, Hajime
Kumai, Reiji
Murakami, Youichi
Takahashi, Hiroki
Matsuishi, Satoru
Hosono, Hideo
author_facet Kobayashi, Kensuke
Yamaura, Jun-ichi
Iimura, Soshi
Maki, Sachiko
Sagayama, Hajime
Kumai, Reiji
Murakami, Youichi
Takahashi, Hiroki
Matsuishi, Satoru
Hosono, Hideo
author_sort Kobayashi, Kensuke
collection PubMed
description A systematic study of the crystal structure of a layered iron oxypnictide LaFeAsO(1−x)H(x) as a function of pressure was performed using synchrotron X-ray diffraction. This compound exhibits a unique phase diagram of two superconducting phases and two parent phases. We established that the As–Fe–As angle of the FeAs(4) tetrahedron widens on the application of pressure due to the interspace between the layers being nearly infilled by the large La and As atoms. Such rarely observed behaviour in iron pnictides implies that the FeAs(4) coordination deviates from the regular tetrahedron in the present systems. This breaks a widely accepted structural guide that the superconductivity favours the regular tetrahedron, albeit the superconducting transition temperature (T(c)) increases from 18 K at ambient pressure to 52 K at 6 GPa for x = 0.2. In the phase diagram, the second parent phase at x ~ 0.5 is suppressed by pressure as low as ~1.5 GPa in contrast to the first parent phase at x ~ 0, which is robust against pressure. We suggest that certain spin-fluctuation from the second parent phase is strongly related to high-T(c) under pressure.
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spelling pubmed-51778812016-12-29 Pressure effect on iron-based superconductor LaFeAsO(1−x)H(x): Peculiar response of 1111-type structure Kobayashi, Kensuke Yamaura, Jun-ichi Iimura, Soshi Maki, Sachiko Sagayama, Hajime Kumai, Reiji Murakami, Youichi Takahashi, Hiroki Matsuishi, Satoru Hosono, Hideo Sci Rep Article A systematic study of the crystal structure of a layered iron oxypnictide LaFeAsO(1−x)H(x) as a function of pressure was performed using synchrotron X-ray diffraction. This compound exhibits a unique phase diagram of two superconducting phases and two parent phases. We established that the As–Fe–As angle of the FeAs(4) tetrahedron widens on the application of pressure due to the interspace between the layers being nearly infilled by the large La and As atoms. Such rarely observed behaviour in iron pnictides implies that the FeAs(4) coordination deviates from the regular tetrahedron in the present systems. This breaks a widely accepted structural guide that the superconductivity favours the regular tetrahedron, albeit the superconducting transition temperature (T(c)) increases from 18 K at ambient pressure to 52 K at 6 GPa for x = 0.2. In the phase diagram, the second parent phase at x ~ 0.5 is suppressed by pressure as low as ~1.5 GPa in contrast to the first parent phase at x ~ 0, which is robust against pressure. We suggest that certain spin-fluctuation from the second parent phase is strongly related to high-T(c) under pressure. Nature Publishing Group 2016-12-22 /pmc/articles/PMC5177881/ /pubmed/28004768 http://dx.doi.org/10.1038/srep39646 Text en Copyright © 2016, The Author(s) 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
Kobayashi, Kensuke
Yamaura, Jun-ichi
Iimura, Soshi
Maki, Sachiko
Sagayama, Hajime
Kumai, Reiji
Murakami, Youichi
Takahashi, Hiroki
Matsuishi, Satoru
Hosono, Hideo
Pressure effect on iron-based superconductor LaFeAsO(1−x)H(x): Peculiar response of 1111-type structure
title Pressure effect on iron-based superconductor LaFeAsO(1−x)H(x): Peculiar response of 1111-type structure
title_full Pressure effect on iron-based superconductor LaFeAsO(1−x)H(x): Peculiar response of 1111-type structure
title_fullStr Pressure effect on iron-based superconductor LaFeAsO(1−x)H(x): Peculiar response of 1111-type structure
title_full_unstemmed Pressure effect on iron-based superconductor LaFeAsO(1−x)H(x): Peculiar response of 1111-type structure
title_short Pressure effect on iron-based superconductor LaFeAsO(1−x)H(x): Peculiar response of 1111-type structure
title_sort pressure effect on iron-based superconductor lafeaso(1−x)h(x): peculiar response of 1111-type structure
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5177881/
https://www.ncbi.nlm.nih.gov/pubmed/28004768
http://dx.doi.org/10.1038/srep39646
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