Comment on “Microwave vortex dissipation of superconducting Nd−Ce−Cu−O epitaxial films in high magnetic fields”
H. A. Blackstead
DOI 10.1103/PhysRevB.74.066501 · 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
Experimental and theoretical results contained in a paper and in an Erratum by Yeh et al. [Phys. Rev. B 48, 9861 (1993); Phys. Rev. B 56, 5683(E) (1997)] discussing experiments employing a novel sapphire ring resonator to investigate microwave frequency vortex dissipation in thin film Nd1.85Ce0.15CuOx as a function of applied field and temperature are discussed. These authors also claim to have extended the Coffey-Clem [Phys. Rev. Lett. 67, 386 (1991); Physica C 185-189, 1915 (1991); Phys. Rev. B 45, 10527 (1992)] model to include thin-films. The authors’ theoretical results for the surface resistance as a function of applied field and temperature, which as illustrated in their paper were in detailed agreement with the data, are only approximately able to describe the data by scaling the theoretical expressions by unspecified multiplicative factors ∼50. The given theory contains no free scaling parameter. In the Erratum, the theory is still in detailed agreement with the NdCe214 data, although these data have changed by roughly a factor of ∼1∕50 due to a claimed experimental recalibration. No explanation was offered to account for the change in the theory, by ∼1∕50. In addition, the expressions provided for the surface resistance are not correct with obvious nonphysical limits: for example, the normal state surface resistance is independent of the resistivity. The recalibrated data are inconsistent with published results for the surface resistance for superconductors and thin film conductors. Equations for the B=0 surface resistance treatment, purportedly appropriate to a finite grain-size limit, were dimensionally inconsistent in the original paper, and an associated fitting parameter was not specified. A value for this “missing” parameter was given in the Erratum, but evaluation of the revised B=0 surface resistance expression with this parameter fails even to approximate the published B=0 curves. Several results from the work of others were misquoted.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Nd1.85Ce0.15CuOx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Pr1.85Ce0.15CuO4-d Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Generation of a dc voltage by an ac magnetic field in type-II superconductors
similarity 0.93Grigorii P. Mikitik & Ernst Helmut Brandt
Source status unknown — claims are unverified
Asymmetric current-voltage characteristics in type-II superconductors
similarity 0.93Xiuguang Jiang et al.
Source status unknown — claims are unverified
Phonon Screening in High-Temperature Superconductors
similarity 0.92C. C. Homes et al.
Source status unknown — claims are unverified
Origin of the Anomalous Low Temperature Upturn in the Resistivity of the Electron-Doped Cuprate Superconductors
similarity 0.92Y. Dagan et al.
Source status unknown — claims are unverified
Structural distortion and superconductivity in (Nd1−xTbx)1.85Ce0.15CuO4
similarity 0.92M. Braden et al.
Source status unknown — claims are unverified
Electromagnetic Radiation from Vortex Flow in Type-II Superconductors
similarity 0.92L. N. Bulaevskii & E. M. Chudnovsky
Source status unknown — claims are unverified