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Microstructure and Superconducting Properties of Bi-2223 Synthesized via Co-Precipitation Method: Effects of Graphene Nanoparticle Addition
The effects of graphene addition on the phase formation and superconducting properties of (Bi(1.6)Pb(0.4))Sr(2)Ca(2)Cu(3)O(10) (Bi-2223) ceramics synthesized using the co-precipitation method were systematically investigated. Series samples of Bi-2223 were added with different weight percentages (x...
Autores principales: | , , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10420798/ https://www.ncbi.nlm.nih.gov/pubmed/37570515 http://dx.doi.org/10.3390/nano13152197 |
Sumario: | The effects of graphene addition on the phase formation and superconducting properties of (Bi(1.6)Pb(0.4))Sr(2)Ca(2)Cu(3)O(10) (Bi-2223) ceramics synthesized using the co-precipitation method were systematically investigated. Series samples of Bi-2223 were added with different weight percentages (x = 0.0, 0.3, 0.5 and 1.0 wt.%) of graphene nanoparticles. The samples’ phase formations and crystal structures were characterized via X-ray diffraction (XRD), while the superconducting critical temperatures, T(c), were investigated using alternating current susceptibility (ACS). The XRD showed that a high-T(c) phase, Bi-2223, and a small low-T(c) phase, Bi-2212, dominated the samples. The volume fraction of the Bi-2223 phase increased for the sample with x = 0.3 wt.% and 0.5 wt.% of graphene and slightly reduced at x = 1.0 wt.%. The ACS showed that the onset critical temperature, T(c-onset), phase lock-in temperature, T(cj,) and coupling peak temperature, T(P), decreased when graphene was added to the samples. The susceptibility–temperature (χ′-T) and (χ″-T) curves of each sample, where χ′ and χ″ are the real and imaginary parts of the susceptibility, respectively, were obtained. The critical temperature of the pure sample was also measured. |
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