Doping dependence of normal- and superconducting-state transport properties of Nd2−xCexCuO4±y thin films
F. Gollnik, M. Naito
DOI 10.1103/PhysRevB.58.11734 · Physical Review B
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Abstract
The electric and thermomagnetic transport properties of an underdoped, an optimally doped, and an overdoped c-axis oriented, epitaxial Nd2−xCexCuO4±y thin film have been investigated in the temperature range from 4.2 K to 300 K and in magnetic fields up to 11 T oriented perpendicular to the CuO2 planes. In the normal state, the resistivity ρ, Hall coefficient RH, and magnetoresistivity Δρ/ρ(B) can be described quantitatively within a simple two-carrier model if the existence of an electronlike and a holelike band is assumed, where each of the two groups of charge carriers is characterized by a temperature-independent Hall coefficient. A corresponding analysis of the thermoelectric effects appears to be more difficult since they depend on more subtle details of the band structure and the scattering mechanisms. In the superconducting regime, the critical field Bρ*(T) determined from the shift of the resistive transition in an external magnetic field exhibits a positive curvature. In contrast, an analysis of the fluctuation conductivity and the transport entropy of magnetic flux line Sφ consistently gives higher values for the upper critical field Bc2(T). The fluctuation conductivity clearly exhibits two-dimensional scaling behavior, indicating that the quasi-two-dimensional nature of the single-layer compound Nd2−xCexCuO4±y might be responsible for the difference between Bρ*(T) and Bc2(T). The order of magnitude of Sφ is consistent with the predictions of the Ginzburg-Landau theory. We derived material parameters as Bc2(0), the in-plane coherence length ξab(0), the Ginzburg-Landau parameter κ, and the London penetration depth λ(0). We also present experimental data on the Hall effect in the mixed state.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Nd1.85Ce0.15CuO4-y Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 24 | Pressure not reported | unknown |
| Nd1.85Ce0.15CuO4-y Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 19 | Pressure not reported | unknown |
| Nd1.82Ce0.18CuO4-y Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 20 | Pressure not reported | unknown |
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