SUPERCONDUCTING PROPERTIES OF Y1-xTbxBa2Cu3O7-δ AND Y1-xTbxSr2Cu2.7Mo0.3O7-δ
We have investigated the effect of Tb substitution for Y in both YBa 2 Cu 3 O 7-δ and the more stabilized YSr 2 Cu 2.7 Mo 0.3 O 7-δ systems. Adding Mo has been shown to stabilize the Tb -doped systems. The samples of Y 1-x Tb x Ba 2 Cu 3 O 7-δ with x=0.0, 0.1, 0.15, 0.2, 0.3, 0.35, 0.4, 0.5, 0.55, and 0.6, and of Y 1-x Tb x Sr 2 Cu 2.7 Mo 0.3 O 7-δ with x=0.0, 0.2, 0.4, 0.6, and 0.8 have been prepared by the standard solid-state reaction technique. The superconducting transition occurs only with x=0–0.5 for the Ba -based samples, and with x=0–0.8 for the Sr -based samples. The structural parameter identification and phase determination of the samples have been carried out by the Rietveld analysis of the X-ray diffraction patterns, which indicates that Tb does not enter in the structure of the Ba -based 123 phase, while in the Sr -based 123 structure Tb enters in the structure and substitutes for Y . In the Y 1-x Tb x Ba 2 Cu 3 O 7-δ samples, a new secondary TbBaO 3 phase forms; and by increasing the amount of Tb , the secondary phase increases as the Y 123 phase decreases. But, for the Y 1-x Tb x Sr 2 Cu 2.7 Mo 0.3 O 7-δ samples, by increasing the amount of Tb doping, no impurity phase is detected in the XRD patterns. For both groups of samples, by increasing the amount of Tb , the normal resistivity increases, and the metallic behavior of the resistivity changes to semiconducting behavior. The magnetoresistance of Y 1-x Tb x Ba 2 Cu 3 O 7-δ was measured in different magnetic fields. The width of transition for the same values of magnetic field increases with the increase of Tb doping, indicating that with the increase of Tb , grains link weaker due to the increase in the amount of the secondary TbBaO 3 phase. The pinning energy has also been evaluated based on the thermally activated phase creep model.