Critical current density of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 superconductor irradiated with neutron in in-core facilities: rotary rack and dry tube at PUSPATI TRIGA Research Reactor
The effects of neutron irradiation in dry tube (DT) and rotary rack (RR) facilities at PUSPATI TRIGA Reactor on the superconducting properties of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 (Bi-2223) are reported. The samples were prepared via the co-precipitation method and exposed to neutron irradiation in both faci...
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my.uniten.dspace-342922024-10-14T11:18:52Z Critical current density of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 superconductor irradiated with neutron in in-core facilities: rotary rack and dry tube at PUSPATI TRIGA Research Reactor Mujaini M. Ilhamsyah A.B.P. Muhammad-Najib K. Hamid N.A. Awang R. Idris F.M. Bayar A.M.J. Hamzah N.S. Abd-Shukor R. 54982692300 57209134726 57211693040 6604077116 22633544100 6701397678 57190940163 56342017400 7004750914 AC susceptibility Critical current density Dry tube Rotary rack Calcium compounds Copper compounds Critical currents Current density Electric resistance Energy dispersive X ray analysis Lead compounds Neutron irradiation Precipitation (chemical) Radioisotopes Strontium compounds Temperature X ray diffraction analysis 'Dry' [ A.C. susceptibility Bi-2223 Core facilities Critical current density Dry tube Electrical resistances Neutron fluences Rotary rack TRIGA research reactor Bismuth compounds The effects of neutron irradiation in dry tube (DT) and rotary rack (RR) facilities at PUSPATI TRIGA Reactor on the superconducting properties of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 (Bi-2223) are reported. The samples were prepared via the co-precipitation method and exposed to neutron irradiation in both facilities for 0.25�h to 5�h with neutron flux 6.90 � 1012 and 2.75 � 1012 n cm?2�s?1, respectively. The structure, microstructure, radionuclide, electrical resistance, and AC susceptibility were determined. Energy-dispersive X-ray analysis revealed the presence of Zn and Po due to the neutron activation. Gamma spectroscopy analysis showed that neutron irradiation produced 85Sr radionuclide. The electrical resistance showed onset temperature, Tc-onset of 118�K and transport critical current density, Jc-t of 2.14 A cm?2 at 50�K for the non-irradiated sample. AC susceptibility showed that the transition temperature, Tc?? was around 106 to 109�K and 105 to 109�K for samples irradiated in DT and RR facilities, respectively. The lower peak temperature, TpL of the imaginary part of the susceptibility, ?? varied from 88 to 97�K. Sample irradiated for 4�h with neutron fluence of 3.96 � 1016 n cm?2 in RR facility showed the highest Jc-t (15.88 A cm?2 at 50�K). Samples irradiated in RR showed higher Jc-t compared with samples irradiated in DT facility. Neutron irradiation suppressed the transition temperature and Bi-2223 phase, but improved Jc-t by more than six times in DT and seven times in RR facility. The optimal neutron fluence for neutron irradiation in Bi-2223 was between 2.48 � 1016 and 3.96 � 1016 n cm?2. � 2023, The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature. Final 2024-10-14T03:18:52Z 2024-10-14T03:18:52Z 2023 Article 10.1007/s00339-023-06598-x 2-s2.0-85152540277 https://www.scopus.com/inward/record.uri?eid=2-s2.0-85152540277&doi=10.1007%2fs00339-023-06598-x&partnerID=40&md5=ff543ad670dbc89012e9ce2122b7ae86 https://irepository.uniten.edu.my/handle/123456789/34292 129 4 306 Springer Science and Business Media Deutschland GmbH Scopus |
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AC susceptibility Critical current density Dry tube Rotary rack Calcium compounds Copper compounds Critical currents Current density Electric resistance Energy dispersive X ray analysis Lead compounds Neutron irradiation Precipitation (chemical) Radioisotopes Strontium compounds Temperature X ray diffraction analysis 'Dry' [ A.C. susceptibility Bi-2223 Core facilities Critical current density Dry tube Electrical resistances Neutron fluences Rotary rack TRIGA research reactor Bismuth compounds |
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AC susceptibility Critical current density Dry tube Rotary rack Calcium compounds Copper compounds Critical currents Current density Electric resistance Energy dispersive X ray analysis Lead compounds Neutron irradiation Precipitation (chemical) Radioisotopes Strontium compounds Temperature X ray diffraction analysis 'Dry' [ A.C. susceptibility Bi-2223 Core facilities Critical current density Dry tube Electrical resistances Neutron fluences Rotary rack TRIGA research reactor Bismuth compounds Mujaini M. Ilhamsyah A.B.P. Muhammad-Najib K. Hamid N.A. Awang R. Idris F.M. Bayar A.M.J. Hamzah N.S. Abd-Shukor R. Critical current density of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 superconductor irradiated with neutron in in-core facilities: rotary rack and dry tube at PUSPATI TRIGA Research Reactor |
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The effects of neutron irradiation in dry tube (DT) and rotary rack (RR) facilities at PUSPATI TRIGA Reactor on the superconducting properties of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 (Bi-2223) are reported. The samples were prepared via the co-precipitation method and exposed to neutron irradiation in both facilities for 0.25�h to 5�h with neutron flux 6.90 � 1012 and 2.75 � 1012 n cm?2�s?1, respectively. The structure, microstructure, radionuclide, electrical resistance, and AC susceptibility were determined. Energy-dispersive X-ray analysis revealed the presence of Zn and Po due to the neutron activation. Gamma spectroscopy analysis showed that neutron irradiation produced 85Sr radionuclide. The electrical resistance showed onset temperature, Tc-onset of 118�K and transport critical current density, Jc-t of 2.14 A cm?2 at 50�K for the non-irradiated sample. AC susceptibility showed that the transition temperature, Tc?? was around 106 to 109�K and 105 to 109�K for samples irradiated in DT and RR facilities, respectively. The lower peak temperature, TpL of the imaginary part of the susceptibility, ?? varied from 88 to 97�K. Sample irradiated for 4�h with neutron fluence of 3.96 � 1016 n cm?2 in RR facility showed the highest Jc-t (15.88 A cm?2 at 50�K). Samples irradiated in RR showed higher Jc-t compared with samples irradiated in DT facility. Neutron irradiation suppressed the transition temperature and Bi-2223 phase, but improved Jc-t by more than six times in DT and seven times in RR facility. The optimal neutron fluence for neutron irradiation in Bi-2223 was between 2.48 � 1016 and 3.96 � 1016 n cm?2. � 2023, The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature. |
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54982692300 |
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54982692300 Mujaini M. Ilhamsyah A.B.P. Muhammad-Najib K. Hamid N.A. Awang R. Idris F.M. Bayar A.M.J. Hamzah N.S. Abd-Shukor R. |
format |
Article |
author |
Mujaini M. Ilhamsyah A.B.P. Muhammad-Najib K. Hamid N.A. Awang R. Idris F.M. Bayar A.M.J. Hamzah N.S. Abd-Shukor R. |
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Mujaini M. |
title |
Critical current density of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 superconductor irradiated with neutron in in-core facilities: rotary rack and dry tube at PUSPATI TRIGA Research Reactor |
title_short |
Critical current density of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 superconductor irradiated with neutron in in-core facilities: rotary rack and dry tube at PUSPATI TRIGA Research Reactor |
title_full |
Critical current density of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 superconductor irradiated with neutron in in-core facilities: rotary rack and dry tube at PUSPATI TRIGA Research Reactor |
title_fullStr |
Critical current density of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 superconductor irradiated with neutron in in-core facilities: rotary rack and dry tube at PUSPATI TRIGA Research Reactor |
title_full_unstemmed |
Critical current density of (Bi1.6Pb0.4)Sr2Ca2Cu3O10 superconductor irradiated with neutron in in-core facilities: rotary rack and dry tube at PUSPATI TRIGA Research Reactor |
title_sort |
critical current density of (bi1.6pb0.4)sr2ca2cu3o10 superconductor irradiated with neutron in in-core facilities: rotary rack and dry tube at puspati triga research reactor |
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Springer Science and Business Media Deutschland GmbH |
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2024 |
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1814061114791559168 |
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13.211869 |