2010
DOI: 10.1016/j.physc.2010.01.011
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Electrical and thermal properties of bulk superconductors Eu0.95Pr0.05Ba2(Cu1−xMx)3O7−δ (M=Fe, Ni, Zn and Mn)

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Cited by 7 publications
(4 citation statements)
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“…However, with co-doping we observe changes in lattice parameters. The XRD patterns of other rare-earth series are reported in our earlier communications [10,11]. Figure 2 shows the temperature dependence of figure of merit for pristine, Pr-doped as well as co-doped samples of Y0.95Pr0.05Ba2(Cu1-xMx)3O7-δ and it is seen that Z value for pristine sample of YBa2Cu3O7-δ (Y-123) remains almost constant for the temperature range 90<T<200 K. It may be mentioned that one can not estimate Z values below 90K because in this range of temperatures, σ tends to infinity and S tends to zero.…”
Section: Resultsmentioning
confidence: 95%
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“…However, with co-doping we observe changes in lattice parameters. The XRD patterns of other rare-earth series are reported in our earlier communications [10,11]. Figure 2 shows the temperature dependence of figure of merit for pristine, Pr-doped as well as co-doped samples of Y0.95Pr0.05Ba2(Cu1-xMx)3O7-δ and it is seen that Z value for pristine sample of YBa2Cu3O7-δ (Y-123) remains almost constant for the temperature range 90<T<200 K. It may be mentioned that one can not estimate Z values below 90K because in this range of temperatures, σ tends to infinity and S tends to zero.…”
Section: Resultsmentioning
confidence: 95%
“…Thermo-power and thermal conductivity measurements were performed simultaneously using direct pulse method. The experimental details of electrical and thermal measurements are described in our previous communications [9][10][11].…”
Section: Experimental Techniquesmentioning
confidence: 99%
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