Effect of praseodymium on the normal-state and superconducting properties of RBa2Cu3Oy: A comparative study of the role of the Pr ion on R and Ba sites
V. E. Gasumyants, M. V. Elizarova, R. Suryanarayanan
DOI 10.1103/PhysRevB.61.12404 · Physical Review B
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Abstract
We present results of a comparative study of the normal-state and superconducting properties in the RBa2Cu3Oy system with substitutions by Pr for the R and Ba sites. The temperature dependences of the resistivity and thermopower were measured for the SmBa2−xPrxCu3Oy (x=0.0–0.35) samples and analyzed in comparison with data for the Y1−xPrxBa2Cu3Oy system. It was observed that the Pr→Ba substitution affects all the properties of the RBa2Cu3Oy system, both the normal state and superconducting, much stronger compared to the Pr→Y one. This manifests itself in an increasing oxygen content, an orthorhombic-to-tetragonal transition at x=0.3–0.35, a stronger rise of the thermopower value, and a faster Tc drop. The results obtained are analyzed within a phenomenological narrow-band model in order to reveal both common peculiarities and specific features of the Pr influence on the band spectrum parameters in the normal state when substituting for different lattice positions. We have observed that the Pr doping leads to a significant modification of the band spectrum, resulting in a strong band broadening and states localization. At the same time, changes of the total effective width of the conduction band WD and the Tc value in two systems with the different kind of Pr doping are shown to correspond to each other so that the Tc(WD) dependence follows the universal correlation for the YBa2Cu3Oy system with different deviations from stoichiometry. Based on our analysis and in agreement with earlier suggestions, we conclude that the superconductivity suppression in both Pr-doped systems could be mainly attributed to the hybridization between 4f states of the Pr ion and the conduction-band states. In addition, Pr in SmBa2−xPrxCu3Oy on the Ba site acts like other trivalent rare-earth impurities inducing the extra hole filling effect that leads to a stronger Tc suppression compared to Y1−xPrxBa2Cu3Oy.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| SmBa2-xPrxCu3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | midpoint |
| SmBa2Cu3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | midpoint |
| Y1-xPrxBa2Cu3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | midpoint |
| PrBa2Cu3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Nd0.7Pr0.3Ba2Cu3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| NdBa1.7Pr0.3Cu3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 31 | Pressure not reported | unknown |
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