Journal
RESULTS IN PHYSICS
Volume 44, Issue -, Pages -Publisher
ELSEVIER
DOI: 10.1016/j.rinp.2022.106140
Keywords
Critical transition temperature; YBCO; Graphene oxide; Impurities; Magnetic nanoparticles
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Y1Ba2Cu3O7-delta (YBCO) was doped with thermally stable and unstable graphene oxide (TS-GO and TU-GO), and both doping increased the critical transition temperature (TCmid), with the highest TCmid observed in the 0.7%wt. TU-GO doped sample. XRD analysis showed an increase in the CuO2 planar area with TCmid for TS-GO and TU-GO doping. Magnetic manganese oxide nanoparticles were observed in the doped samples, resulting from impurities in the graphene oxide dopant material. Doping with trimanganese tetraoxide (Mn3O4) and manganese dioxide (MnO2) also increased TCmid, but a higher concentration of Mn3O4 led to a decrease in TCmid.
Y1Ba2Cu3O7-delta (YBCO) was doped with thermally stable graphene oxide (TS-GO) and thermally unstable graphene oxide (TU-GO) in the following %wt. concentrations: 0.1, 0.5 and 0.7. TS-GO and TU-GO was characterized using RAMAN, fourier transform infrared spectroscopy (FTIR) and energy-dispersive X-ray spectroscopy (EDX). The critical transition temperature (TCmid) increased in all TU-GO and TS-GO doped samples. The highest TCmid of 101 K was that of the 0.7 %wt. TU-GO doped sample. The increase in TCmid was greater for the samples doped with TU-GO. Non-stoichiometric oxygen content (delta) was seen to increase with an increase in doping concen-tration of both TS-GO and TU-GO. X-ray diffraction (XRD) analysis was carried out to determine the lattice parameters and phase characterization of the TU-GO and TS-GO doped samples. Lattice parameters show an increase in the copper oxide (CuO2) planar area with TCmid for TS-GO and TU-GO doping. To determine strain effects, the Williamson Hall method was used to determine the lattice strain (epsilon). The epsilon was seen to decrease for both TS-GO and TU-GO doped samples. The formation of magnetic manganese oxide nanoparticles in TS-GO and TU-GO doped samples was observed, and resulted from impurities found in the graphene oxide (GO) dopant material. The magnetic particles were extracted magnetically and characterized using EDX. YBCO was doped with trimanganese tetraoxide (Mn3O4) and manganese dioxide (MnO2) in a 0.1 and 0.2 %wt. concentration. The TCmid is seen to increase to 94 K and 104 K respectively for 0.1 %wt. MnO2 and Mn3O4 doped samples. The 0.2 % wt. doped Mn3O4 sample resulted in a decrease in TCmid. Magnetic susceptibility measurements confirmed a superconducting phase changes. The increase in TCmid above YBCO's Tc = 93 K, correlates to the presence of manganese nano-impurities. This increase is hypothezied to be related to an increase in surface area of YBCO's 2D copper oxide (CuO2) plane structure with GO doping.
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