Structural analysis of the [RE.sub.3][Ba.sub.5][Cu.sub.8][O.sub.18]
In this paper, we report the synthesis and structural characterization of the [RE.sub.3][Ba.sub.5][Cu.sub.8][O.sub.18] (RE = Dy, Gd, Ho, Sm, Y, Yb) system, which adds to the findings reported by Aliabadi, et al., who determined a critical temperature ([T.sub.C]) of ~ 100 K for the superconducting [Y...
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Veröffentlicht in: | Revista de la Academia colombiana de ciencias exactas, físicas y naturales físicas y naturales, 2021-01, Vol.45 (174), p.83 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | In this paper, we report the synthesis and structural characterization of the [RE.sub.3][Ba.sub.5][Cu.sub.8][O.sub.18] (RE = Dy, Gd, Ho, Sm, Y, Yb) system, which adds to the findings reported by Aliabadi, et al., who determined a critical temperature ([T.sub.C]) of ~ 100 K for the superconducting [Y.sub.3][Ba.sub.5][Cu.sub.8][O.sub.18] system and evaluated its structural response in a sample. The new [RE.sub.3][Ba.sub.5][Cu.sub.8][O.sub.18] system was produced using the solidstate reaction method and a similar thermal process as the one used for the superconductor RE: 123. The experimental results obtained with X-ray diffraction and the Rietveld analysis showed that these samples had the expected crystal structure. However, it was obvious that the presence of non-superconducting phases did not affect the superconducting transition temperature. Moreover, magnetic studies revealed that [RE.sub.3][Ba.sub.5][Cu.sub.8][O.sub.18] samples showed a superconductivity transition within a temperature range of 80 - 93 K depending on the rare earth. |
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ISSN: | 0370-3908 |
DOI: | 10.18257/raccefyn.1163 |