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Evolution of two bulk-superconducting phases in Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, Sm) by external hydrostatic pressure effect

Polycrystalline samples of Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, and Sm) were synthesized via the solid-state reaction and characterized using synchrotron X-ray diffraction. Although all the Sr(0.5)RE(0.5)FBiS(2) samples exhibited superconductivity at transition temperatures (T(c)) within the r...

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Autores principales: Yamashita, Aichi, Jha, Rajveer, Goto, Yosuke, Miura, Akira, Moriyoshi, Chikako, Kuroiwa, Yoshihiro, Kawashima, Chizuru, Ishida, Kouhei, Takahashi, Hiroki, Mizuguchi, Yoshikazu
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7393496/
https://www.ncbi.nlm.nih.gov/pubmed/32732897
http://dx.doi.org/10.1038/s41598-020-69889-w
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author Yamashita, Aichi
Jha, Rajveer
Goto, Yosuke
Miura, Akira
Moriyoshi, Chikako
Kuroiwa, Yoshihiro
Kawashima, Chizuru
Ishida, Kouhei
Takahashi, Hiroki
Mizuguchi, Yoshikazu
author_facet Yamashita, Aichi
Jha, Rajveer
Goto, Yosuke
Miura, Akira
Moriyoshi, Chikako
Kuroiwa, Yoshihiro
Kawashima, Chizuru
Ishida, Kouhei
Takahashi, Hiroki
Mizuguchi, Yoshikazu
author_sort Yamashita, Aichi
collection PubMed
description Polycrystalline samples of Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, and Sm) were synthesized via the solid-state reaction and characterized using synchrotron X-ray diffraction. Although all the Sr(0.5)RE(0.5)FBiS(2) samples exhibited superconductivity at transition temperatures (T(c)) within the range of 2.1–2.7 K under ambient pressure, the estimated superconducting volume fraction was small, which indicates non-bulk nature of superconductivity in those samples under ambient pressure. A dramatic increase in shielding fraction, which indicates the emergence of the bulk superconductivity was achieved by applying external hydrostatic pressures. We found that two phases, low-P phases with T(c) = 2.5–2.8 K and high-P phases with T(c) = 10.0–10.8 K, were induced by the pressure effect for samples with RE = La, Ce, Pr, and Nd. Pressure-T(c) phase diagrams indicated that the critical pressure for the emergence of the high-P phase tends to increase with decreasing ionic radius of the doped RE ions, which was explained by the correlation between external and chemical pressure effects. According to the high-pressure X-ray diffraction measurements of Sr(0.5)La(0.5)FBiS(2), a structural phase transition from tetragonal to monoclinic also occurred at approximately 1.1 GPa. Bulk superconducting phases in Sr(0.5)RE(0.5)FBiS(2) induced by the external hydrostatic pressure effect are expected to be useful for understanding the effects of both external and chemical pressures to the emergence of bulk superconductivity and pairing mechanisms in BiCh(2)-based superconductors.
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spelling pubmed-73934962020-08-03 Evolution of two bulk-superconducting phases in Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, Sm) by external hydrostatic pressure effect Yamashita, Aichi Jha, Rajveer Goto, Yosuke Miura, Akira Moriyoshi, Chikako Kuroiwa, Yoshihiro Kawashima, Chizuru Ishida, Kouhei Takahashi, Hiroki Mizuguchi, Yoshikazu Sci Rep Article Polycrystalline samples of Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, and Sm) were synthesized via the solid-state reaction and characterized using synchrotron X-ray diffraction. Although all the Sr(0.5)RE(0.5)FBiS(2) samples exhibited superconductivity at transition temperatures (T(c)) within the range of 2.1–2.7 K under ambient pressure, the estimated superconducting volume fraction was small, which indicates non-bulk nature of superconductivity in those samples under ambient pressure. A dramatic increase in shielding fraction, which indicates the emergence of the bulk superconductivity was achieved by applying external hydrostatic pressures. We found that two phases, low-P phases with T(c) = 2.5–2.8 K and high-P phases with T(c) = 10.0–10.8 K, were induced by the pressure effect for samples with RE = La, Ce, Pr, and Nd. Pressure-T(c) phase diagrams indicated that the critical pressure for the emergence of the high-P phase tends to increase with decreasing ionic radius of the doped RE ions, which was explained by the correlation between external and chemical pressure effects. According to the high-pressure X-ray diffraction measurements of Sr(0.5)La(0.5)FBiS(2), a structural phase transition from tetragonal to monoclinic also occurred at approximately 1.1 GPa. Bulk superconducting phases in Sr(0.5)RE(0.5)FBiS(2) induced by the external hydrostatic pressure effect are expected to be useful for understanding the effects of both external and chemical pressures to the emergence of bulk superconductivity and pairing mechanisms in BiCh(2)-based superconductors. Nature Publishing Group UK 2020-07-30 /pmc/articles/PMC7393496/ /pubmed/32732897 http://dx.doi.org/10.1038/s41598-020-69889-w Text en © The Author(s) 2020 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Yamashita, Aichi
Jha, Rajveer
Goto, Yosuke
Miura, Akira
Moriyoshi, Chikako
Kuroiwa, Yoshihiro
Kawashima, Chizuru
Ishida, Kouhei
Takahashi, Hiroki
Mizuguchi, Yoshikazu
Evolution of two bulk-superconducting phases in Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, Sm) by external hydrostatic pressure effect
title Evolution of two bulk-superconducting phases in Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, Sm) by external hydrostatic pressure effect
title_full Evolution of two bulk-superconducting phases in Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, Sm) by external hydrostatic pressure effect
title_fullStr Evolution of two bulk-superconducting phases in Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, Sm) by external hydrostatic pressure effect
title_full_unstemmed Evolution of two bulk-superconducting phases in Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, Sm) by external hydrostatic pressure effect
title_short Evolution of two bulk-superconducting phases in Sr(0.5)RE(0.5)FBiS(2) (RE: La, Ce, Pr, Nd, Sm) by external hydrostatic pressure effect
title_sort evolution of two bulk-superconducting phases in sr(0.5)re(0.5)fbis(2) (re: la, ce, pr, nd, sm) by external hydrostatic pressure effect
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7393496/
https://www.ncbi.nlm.nih.gov/pubmed/32732897
http://dx.doi.org/10.1038/s41598-020-69889-w
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