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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...

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Detalles Bibliográficos
Autores principales: Abdullah, Siti Nabilah, Kechik, Mohd Mustafa Awang, Kamarudin, Aliah Nursyahirah, Talib, Zainal Abidin, Baqiah, Hussein, Kien, Chen Soo, Pah, Lim Kean, Abdul Karim, Muhammad Khalis, Shabdin, Muhammad Kashfi, Shaari, Abdul Halim, Hashim, Azhan, Suhaimi, Nurbaisyatul Ermiza, Miryala, Muralidhar
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
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
Descripción
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.