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Bulk superconductivity in a four-layer-type Bi-based compound La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3)

Recently, we reported the observation of superconductivity at ~0.5 K in a La(2)O(2)M(4)S(6)-type (M: metal) layered compound La(2)O(2)Bi(3)AgS(6), which is a layered system related to the BiS(2)-based superconductor system but possesses a thicker Bi(3)AgS(6)-type conducting layer. In this study, we...

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Autores principales: Jha, Rajveer, Goto, Yosuke, Matsuda, Tatsuma D., Aoki, Yuji, Nagao, Masanori, Tanaka, Isao, Mizuguchi, Yoshikazu
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6753103/
https://www.ncbi.nlm.nih.gov/pubmed/31537836
http://dx.doi.org/10.1038/s41598-019-49934-z
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author Jha, Rajveer
Goto, Yosuke
Matsuda, Tatsuma D.
Aoki, Yuji
Nagao, Masanori
Tanaka, Isao
Mizuguchi, Yoshikazu
author_facet Jha, Rajveer
Goto, Yosuke
Matsuda, Tatsuma D.
Aoki, Yuji
Nagao, Masanori
Tanaka, Isao
Mizuguchi, Yoshikazu
author_sort Jha, Rajveer
collection PubMed
description Recently, we reported the observation of superconductivity at ~0.5 K in a La(2)O(2)M(4)S(6)-type (M: metal) layered compound La(2)O(2)Bi(3)AgS(6), which is a layered system related to the BiS(2)-based superconductor system but possesses a thicker Bi(3)AgS(6)-type conducting layer. In this study, we have developed the La(2)O(2)Bi(3)AgS(6)-type materials by element substitutions to increase the transition temperature (T(c)) and to induce bulk nature of superconductivity. A resistivity anomaly observed at 180 K in La(2)O(2)Bi(3)AgS(6) was systematically suppressed by Sn substitution for the Ag site. By the Sn substitution, T(c) increased, and the shielding volume fraction estimated from magnetization measurements also increased. The highest T(c) (=2.3 K) and the highest shielding volume fraction (~20%) was observed for La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(6). The superconducting properties were further improved by Se substitutions for the S site. By the combinational substitutions of Sn and Se, bulk-superconducting phase of La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3) with a T(c) of 3.0 K (T(c)(onset) = 3.6 K) was obtained.
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spelling pubmed-67531032019-10-01 Bulk superconductivity in a four-layer-type Bi-based compound La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3) Jha, Rajveer Goto, Yosuke Matsuda, Tatsuma D. Aoki, Yuji Nagao, Masanori Tanaka, Isao Mizuguchi, Yoshikazu Sci Rep Article Recently, we reported the observation of superconductivity at ~0.5 K in a La(2)O(2)M(4)S(6)-type (M: metal) layered compound La(2)O(2)Bi(3)AgS(6), which is a layered system related to the BiS(2)-based superconductor system but possesses a thicker Bi(3)AgS(6)-type conducting layer. In this study, we have developed the La(2)O(2)Bi(3)AgS(6)-type materials by element substitutions to increase the transition temperature (T(c)) and to induce bulk nature of superconductivity. A resistivity anomaly observed at 180 K in La(2)O(2)Bi(3)AgS(6) was systematically suppressed by Sn substitution for the Ag site. By the Sn substitution, T(c) increased, and the shielding volume fraction estimated from magnetization measurements also increased. The highest T(c) (=2.3 K) and the highest shielding volume fraction (~20%) was observed for La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(6). The superconducting properties were further improved by Se substitutions for the S site. By the combinational substitutions of Sn and Se, bulk-superconducting phase of La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3) with a T(c) of 3.0 K (T(c)(onset) = 3.6 K) was obtained. Nature Publishing Group UK 2019-09-19 /pmc/articles/PMC6753103/ /pubmed/31537836 http://dx.doi.org/10.1038/s41598-019-49934-z Text en © The Author(s) 2019 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
Jha, Rajveer
Goto, Yosuke
Matsuda, Tatsuma D.
Aoki, Yuji
Nagao, Masanori
Tanaka, Isao
Mizuguchi, Yoshikazu
Bulk superconductivity in a four-layer-type Bi-based compound La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3)
title Bulk superconductivity in a four-layer-type Bi-based compound La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3)
title_full Bulk superconductivity in a four-layer-type Bi-based compound La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3)
title_fullStr Bulk superconductivity in a four-layer-type Bi-based compound La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3)
title_full_unstemmed Bulk superconductivity in a four-layer-type Bi-based compound La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3)
title_short Bulk superconductivity in a four-layer-type Bi-based compound La(2)O(2)Bi(3)Ag(0.6)Sn(0.4)S(5.7)Se(0.3)
title_sort bulk superconductivity in a four-layer-type bi-based compound la(2)o(2)bi(3)ag(0.6)sn(0.4)s(5.7)se(0.3)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6753103/
https://www.ncbi.nlm.nih.gov/pubmed/31537836
http://dx.doi.org/10.1038/s41598-019-49934-z
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