Preparation and characterization of a new graphite superconductor: Ca0.5Sr0.5C6

Abstract We have produced a superconducting binary-elements intercalated graphite, CaxSr1−xCy, with the intercalation of Sr and Ca in highly-oriented pyrolytic graphite; the superconducting transition temperature, T c, was ~3 K. The superconducting CaxSr1−xCy sample was fabricated with the nominal x...

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Autores principales: Saki Nishiyama, Hidenori Fujita, Masatoshi Hoshi, Xiao Miao, Takahiro Terao, Xiaofan Yang, Takafumi Miyazaki, Hidenori Goto, Tomoko Kagayama, Katsuya Shimizu, Hitoshi Yamaoka, Hirofumi Ishii, Yen-Fa Liao, Yoshihiro Kubozono
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Publicado: Nature Portfolio 2017
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spelling oai:doaj.org-article:f6d80f7f5cda4b67b28dc6872c51f58f2021-12-02T15:05:11ZPreparation and characterization of a new graphite superconductor: Ca0.5Sr0.5C610.1038/s41598-017-07763-y2045-2322https://doaj.org/article/f6d80f7f5cda4b67b28dc6872c51f58f2017-08-01T00:00:00Zhttps://doi.org/10.1038/s41598-017-07763-yhttps://doaj.org/toc/2045-2322Abstract We have produced a superconducting binary-elements intercalated graphite, CaxSr1−xCy, with the intercalation of Sr and Ca in highly-oriented pyrolytic graphite; the superconducting transition temperature, T c, was ~3 K. The superconducting CaxSr1−xCy sample was fabricated with the nominal x value of 0.8, i.e., Ca0.8Sr0.2Cy. Energy dispersive X-ray (EDX) spectroscopy provided the stoichiometry of Ca0.5(2)Sr0.5(2)Cy for this sample, and the X-ray powder diffraction (XRD) pattern showed that Ca0.5(2)Sr0.5(2)Cy took the SrC6-type hexagonal-structure rather than CaC6-type rhombohedral-structure. Consequently, the chemical formula of CaxSr1−xCy sample could be expressed as ‘Ca0.5(2)Sr0.5(2)C6’. The XRD pattern of Ca0.5(2)Sr0.5(2)C6 was measured at 0–31 GPa, showing that the lattice shrank monotonically with increasing pressure up to 8.6 GPa, with the structural phase transition occurring above 8.6 GPa. The pressure dependence of T c was determined from the DC magnetic susceptibility and resistance up to 15 GPa, which exhibited a positive pressure dependence of T c up to 8.3 GPa, as in YbC6, SrC6, KC8, CaC6 and Ca0.6K0.4C8. The further application of pressure caused the rapid decrease of T c. In this study, the fabrication and superconducting properties of new binary-elements intercalated graphite, CaxSr1−xCy, are fully investigated, and suitable combinations of elements are suggested for binary-elements intercalated graphite.Saki NishiyamaHidenori FujitaMasatoshi HoshiXiao MiaoTakahiro TeraoXiaofan YangTakafumi MiyazakiHidenori GotoTomoko KagayamaKatsuya ShimizuHitoshi YamaokaHirofumi IshiiYen-Fa LiaoYoshihiro KubozonoNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 7, Iss 1, Pp 1-10 (2017)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Saki Nishiyama
Hidenori Fujita
Masatoshi Hoshi
Xiao Miao
Takahiro Terao
Xiaofan Yang
Takafumi Miyazaki
Hidenori Goto
Tomoko Kagayama
Katsuya Shimizu
Hitoshi Yamaoka
Hirofumi Ishii
Yen-Fa Liao
Yoshihiro Kubozono
Preparation and characterization of a new graphite superconductor: Ca0.5Sr0.5C6
description Abstract We have produced a superconducting binary-elements intercalated graphite, CaxSr1−xCy, with the intercalation of Sr and Ca in highly-oriented pyrolytic graphite; the superconducting transition temperature, T c, was ~3 K. The superconducting CaxSr1−xCy sample was fabricated with the nominal x value of 0.8, i.e., Ca0.8Sr0.2Cy. Energy dispersive X-ray (EDX) spectroscopy provided the stoichiometry of Ca0.5(2)Sr0.5(2)Cy for this sample, and the X-ray powder diffraction (XRD) pattern showed that Ca0.5(2)Sr0.5(2)Cy took the SrC6-type hexagonal-structure rather than CaC6-type rhombohedral-structure. Consequently, the chemical formula of CaxSr1−xCy sample could be expressed as ‘Ca0.5(2)Sr0.5(2)C6’. The XRD pattern of Ca0.5(2)Sr0.5(2)C6 was measured at 0–31 GPa, showing that the lattice shrank monotonically with increasing pressure up to 8.6 GPa, with the structural phase transition occurring above 8.6 GPa. The pressure dependence of T c was determined from the DC magnetic susceptibility and resistance up to 15 GPa, which exhibited a positive pressure dependence of T c up to 8.3 GPa, as in YbC6, SrC6, KC8, CaC6 and Ca0.6K0.4C8. The further application of pressure caused the rapid decrease of T c. In this study, the fabrication and superconducting properties of new binary-elements intercalated graphite, CaxSr1−xCy, are fully investigated, and suitable combinations of elements are suggested for binary-elements intercalated graphite.
format article
author Saki Nishiyama
Hidenori Fujita
Masatoshi Hoshi
Xiao Miao
Takahiro Terao
Xiaofan Yang
Takafumi Miyazaki
Hidenori Goto
Tomoko Kagayama
Katsuya Shimizu
Hitoshi Yamaoka
Hirofumi Ishii
Yen-Fa Liao
Yoshihiro Kubozono
author_facet Saki Nishiyama
Hidenori Fujita
Masatoshi Hoshi
Xiao Miao
Takahiro Terao
Xiaofan Yang
Takafumi Miyazaki
Hidenori Goto
Tomoko Kagayama
Katsuya Shimizu
Hitoshi Yamaoka
Hirofumi Ishii
Yen-Fa Liao
Yoshihiro Kubozono
author_sort Saki Nishiyama
title Preparation and characterization of a new graphite superconductor: Ca0.5Sr0.5C6
title_short Preparation and characterization of a new graphite superconductor: Ca0.5Sr0.5C6
title_full Preparation and characterization of a new graphite superconductor: Ca0.5Sr0.5C6
title_fullStr Preparation and characterization of a new graphite superconductor: Ca0.5Sr0.5C6
title_full_unstemmed Preparation and characterization of a new graphite superconductor: Ca0.5Sr0.5C6
title_sort preparation and characterization of a new graphite superconductor: ca0.5sr0.5c6
publisher Nature Portfolio
publishDate 2017
url https://doaj.org/article/f6d80f7f5cda4b67b28dc6872c51f58f
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