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 (Bi1.6Pb0.4)Sr2Ca2Cu3O10 (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,...

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Bibliographic Details
Published in:Nanomaterials
Main Author: Abdullah S.N.; Kechik M.M.A.; Kamarudin A.N.; Talib Z.A.; Baqiah H.; Kien C.S.; Pah L.K.; Abdul Karim M.K.; Shabdin M.K.; Shaari A.H.; Hashim A.; Suhaimi N.E.; Miryala M.
Format: Article
Language:English
Published: Multidisciplinary Digital Publishing Institute (MDPI) 2023
Online Access:https://www.scopus.com/inward/record.uri?eid=2-s2.0-85167719245&doi=10.3390%2fnano13152197&partnerID=40&md5=b8bb163b1f352ca422e96b0a63af0714
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Summary:The effects of graphene addition on the phase formation and superconducting properties of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 (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, Tc, were investigated using alternating current susceptibility (ACS). The XRD showed that a high-Tc phase, Bi-2223, and a small low-Tc 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, Tc-onset, phase lock-in temperature, Tcj, and coupling peak temperature, TP, 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. © 2023 by the authors.
ISSN:20794991
DOI:10.3390/nano13152197