Thermal and electronic properties of rare-earth Ba2Cu3Ox superconductors
J. Heremans, D. T. Morelli, G. W. Smith, S. C. Strite III
DOI 10.1103/PhysRevB.37.1604 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
We have measured the electrical resistivity, thermal conductivity, and specific heat of a series of high-temperature superconducting compounds of the form RBa2Cu3O7, with R=Y, Eu, Gd, Dy, and Er. Our results show that the afore-mentioned physical properties are virtually identical for all samples considered. In particular, the molar specific heats are identical to within ±2% and exhibit Debye-type behavior. We observe a nearly constant thermal conductivity above Tc, but a rather sudden increase developes as the temperature is lowered below the critical temperature. The electrical resistivity is nearly linear in the normal state. Thermal and electrical conductivities indicate that for T>Tc, the predominant electron scattering mechanism is due to phonon interactions. Using electrical resistivity data and the Wiedemann-Franz law, we estimate the magnitude of the electronic component of the thermal conductivity to be an order of magnitude smaller than the measured thermal conductivity. We thus conclude that heat transport is predominantly by phonons. The enhancement of the lattice conduction below the critical temperature is understood as a reduction of carrier-phonon scattering as electrons condense into Cooper pairs. This lends support to standard Bardeen-Cooper-Schrieffer-type superconductivity. An estimate of the superconducting transition temperatures is made using the electron-phonon coupling constants and Debye temperatures deduced from the data which brackets the observed Tc quite well. We discuss the thermal conductivity at very low temperature in terms of a phonon mean-free path limited by pores in the samples.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| GdBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 89.4 | Pressure not reported | zero_resistance |
| DyBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 87.1 | Pressure not reported | zero_resistance |
| EuBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 83.2 | Pressure not reported | zero_resistance |
| YBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 86 | Pressure not reported | zero_resistance |
| ErBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90 | Pressure not reported | zero_resistance |
Similar papers
Superconductivity in sulfur-containing R-Ba-Cu-O compounds
similarity 0.97R. Gagnon et al.
Source status unknown — claims are unverified
Superconducting fluctuations in the thermal conductivity of Bi2Sr2CaCu2O8 and DyBa2Cu3O7−x materials
similarity 0.97M. Houssa et al.
Source status unknown — claims are unverified
Long-range magnetic ordering in the high-Tc superconductors RBa2Cu3O7−δ (R=Nd, Sm, Gd, Dy, and Er)
similarity 0.97B. W. Lee et al.
Source status unknown — claims are unverified
Thermal conductivity of impurity-doped high-Tc superconductors
similarity 0.97S. T. Ting et al.
Source status unknown — claims are unverified
Structural properties of Ba2RCu3O7 high-Tc superconductors
similarity 0.97Y. Le Page et al.
Source status unknown — claims are unverified
Magnetic relaxation in sintered Tl2Ca2Ba2Cu3Ox and YBa2Cu3O7−x superconductors
similarity 0.97M. E. McHenry et al.
Source status unknown — claims are unverified