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Increased flux pinning force and critical current density in MgB(2) by nano-La(2)O(3) doping

MgB(2) superconducting wires and bulks with nano-La(2)O(3) addition have been studied. A series of MgB(2) superconducting bulk samples with nano-La(2)O(3) addition levels of 0, 5, 7, 18wt% were prepared. AC resistivity data showed slight increases of Bc(2) and unchanged B(irr) for the bulk samples w...

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Detalles Bibliográficos
Autores principales: Zhang, Danlu, Wan, Fang, Sumption, Michael D., Collings, Edward W., Thong, CJ, Rindfleisch, Matt, Tomsic, Mike
Formato: Online Artículo Texto
Lenguaje:English
Publicado: 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8547606/
https://www.ncbi.nlm.nih.gov/pubmed/34707692
http://dx.doi.org/10.1088/1757-899x/756/1/012019
Descripción
Sumario:MgB(2) superconducting wires and bulks with nano-La(2)O(3) addition have been studied. A series of MgB(2) superconducting bulk samples with nano-La(2)O(3) addition levels of 0, 5, 7, 18wt% were prepared. AC resistivity data showed slight increases of Bc(2) and unchanged B(irr) for the bulk samples with doping levels lower than 7 wt% and decreased critical fields for the heavily doped (18 wt%) bulk. X-ray diffraction (XRD) showed the presence of LaB(6) in the nano-La(2)O(3) doped MgB(2) bulk samples and decreased MgB(2) grain size in nano-La(2)O(3) doped bulks. Monocore powder-in-tube (PIT) MgB(2) wires without and with 5 wt% nano-La(2)O(3) addition (P-05) were prepared for transport property measurement. 2mol%C-doped Specialty Materials Inc. (SMI) boron powder was used for wire P-05 and previously prepared control wires (control wires were made without the addition of nano-La(2)O(3) powder, W-00 and P2). Low field magnetic properties were obtained from magnetization loop (M–H), transport critical current density (J(c)) was measured at 4.2 K for the nano-La(2)O(3) doped PIT wire (P-05) and the control samples (P2 and W-00). The transport critical current density J(c) (B) of P-05 at 4.2 K and 8 T (6.0 ×10(4) A/cm(2)) was twice that of the control wire. The critical magnetic fields (Bc(2) and B(irr)) of P-05 and the control sample P2 were compared. The critical fields of P-05 were slightly less than those of P2. Kramer-Dew-Hughes plots indicated a change from surface pinning to a mixture of volume pinning and surface pinning. It is shown that enhancement of P-05’s transport properties is due to additional flux pinning by the fine-size rare-earth borides rather than enhanced Bc(2) or B(irr).