TY - JOUR
T1 - Optimization of Carbon Encapsulated Boron Doping for High-Performance Bulk Sintered MgB2
AU - Sai Srikanth, Arvapalli
AU - Muralidhar, Miryala
AU - Sunsanee, Pinmangkorn
AU - Jirsa, Milos
AU - Sakai, Naomichi
AU - Oka, Tetsuo
AU - Murakami, Masato
N1 - Funding Information:
S.S.A. and P.S. would like to acknowledge Shibaura Institute of Technology (SIT), Tokyo, Japan, for providing the financial support for the doctoral program.
Publisher Copyright:
© 2020 The Authors. Published by WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
PY - 2020/11
Y1 - 2020/11
N2 - Carbon has been a standard doping agent in MgB2 for long time. It, however, has also participated in a non-uniform distribution of the constituents throughout the bulk MgB2. To address this issue, carbon encapsulated boron (CEB) was used instead of the manually added mixture of boron and carbon. The previous studies confirmed that only low concentrations of carbon in CEB were effective for synthesis of a high-performance bulk MgB2. Here, a further step in optimization carbon content in CEB is reported. Carbon content in CEB varied as 1, 1.1, 1.35, 1.5, and 1.9 wt%. X-ray diffraction (XRD) results depict a slight shift in peaks corresponding to a–b plane, indicating carbon substitution into the lattice. High superconducting critical current density in self-field, such as 660, 550, and 435 kA cm−2, was observed in the samples with 1.5 wt% CEB at 10, 15, and 20 K, respectively. In addition, Jc of 75 kA cm−2 at 2 T and 20 K was observed in the 1.5 wt% CEB sample, which is thrice the value observed in the pure sample, with a minute tradeoff in Tc (around 37.5 K). Scanning electron microscope (SEM) images reveal that small particles of size ranging from 50 to 200 nm contribute to Jc improvement. Energy-dispersive X-ray (EDX) results show carbon uniformly distributed throughout the bulk.
AB - Carbon has been a standard doping agent in MgB2 for long time. It, however, has also participated in a non-uniform distribution of the constituents throughout the bulk MgB2. To address this issue, carbon encapsulated boron (CEB) was used instead of the manually added mixture of boron and carbon. The previous studies confirmed that only low concentrations of carbon in CEB were effective for synthesis of a high-performance bulk MgB2. Here, a further step in optimization carbon content in CEB is reported. Carbon content in CEB varied as 1, 1.1, 1.35, 1.5, and 1.9 wt%. X-ray diffraction (XRD) results depict a slight shift in peaks corresponding to a–b plane, indicating carbon substitution into the lattice. High superconducting critical current density in self-field, such as 660, 550, and 435 kA cm−2, was observed in the samples with 1.5 wt% CEB at 10, 15, and 20 K, respectively. In addition, Jc of 75 kA cm−2 at 2 T and 20 K was observed in the 1.5 wt% CEB sample, which is thrice the value observed in the pure sample, with a minute tradeoff in Tc (around 37.5 K). Scanning electron microscope (SEM) images reveal that small particles of size ranging from 50 to 200 nm contribute to Jc improvement. Energy-dispersive X-ray (EDX) results show carbon uniformly distributed throughout the bulk.
KW - bulk MgB
KW - carbon encapsulated boron
KW - optimization
KW - sintering
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U2 - 10.1002/adem.202000478
DO - 10.1002/adem.202000478
M3 - Article
AN - SCOPUS:85087164819
SN - 1438-1656
VL - 22
JO - Advanced Engineering Materials
JF - Advanced Engineering Materials
IS - 11
M1 - 2000478
ER -