Microstructure and Superconducting Properties of Bi-2223 Synthesized via Co-Precipitation Method: Effects of Graphene Nanoparticle Addition

Author:

Abdullah Siti Nabilah1,Kechik Mohd Mustafa Awang1ORCID,Kamarudin Aliah Nursyahirah1,Talib Zainal Abidin2,Baqiah Hussein3,Kien Chen Soo1ORCID,Pah Lim Kean1ORCID,Abdul Karim Muhammad Khalis1ORCID,Shabdin Muhammad Kashfi1,Shaari Abdul Halim1,Hashim Azhan4,Suhaimi Nurbaisyatul Ermiza4,Miryala Muralidhar5ORCID

Affiliation:

1. Laboratory of Superconductor and Thin Films, Department of Physics, Faculty of Science, Universiti Putra Malaysia, Serdang 43400, Malaysia

2. Department of Physics, College of Natural Sciences, Jeonbuk National University 567, Baekje-daero, Deokjin-gu, Jeonju-si 54896, Republic of Korea

3. Shandong Key Laboratory of Biophysics, Institute of Biophysics, Dezhou University, No. 566 University Rd. West, Dezhou 253023, China

4. Faculty of Applied Sciences, Universiti Teknologi MARA Pahang, Jengka 26400, Malaysia

5. Materials for Energy and Environmental Laboratory, Superconducting Materials, Shibaura Institute of Technology, 3 Chome-7-5 Toyosu, Koto, Tokyo 135-8548, Japan

Abstract

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.

Funder

Ministry of Higher Education

Publisher

MDPI AG

Subject

General Materials Science,General Chemical Engineering

Reference69 articles.

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