D. Fay
University of Hamburg
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Featured researches published by D. Fay.
Solid State Communications | 1988
L. Tewordt; D. Fay; Th. Wölkhausen
Abstract The fluctuation conductivity and specific heat are derived from the Aslamazov-Larkin theory by taking into account the quasi two-dimensionality of the effective tight-binding band. The resulting coherence lengths in the basal plane are calculated explicitly for the Hubbard models of Emery and Mattis and Mattis. They turn out to depend sensitively on band width, band filling, impurity scattering rate, and pair state ( s -wave, d -wave, and uniaxial s - d -wave). Small band dispersion along the c -axis yields 2D to 3D crossover as T → T c . Our theory is capable of accounting for the small coherence lengths derived from measurements of H c 2 , the fluctuation conductivity, and the specific heat in YBa 2 Cu 3 O 7 . We suggest measurements of the fluctuation conductivity at microwave or infrared frequencies.
Physical Review B | 2001
L. Tewordt; D. Fay
We calculate the thermal conductivity
Physical Review B | 2003
L. Tewordt; D. Fay
\ensuremath{\kappa}
Solid State Communications | 1974
Arthur Layzer; D. Fay
in magnetic fields near
Journal of Low Temperature Physics | 1978
L. Tewordt; D. Fay; N. Schopohl
{H}_{c2}
Physical Review B | 2005
L. Tewordt; D. Fay
for spin-triplet superconducting states with line nodes vertical and horizontal relative to the
Physical Review B | 2001
D. Fay; J. Appel; Carsten Timm; Andreas Zabel
{\mathrm{RuO}}_{2}
Physical Review B | 2000
D. Fay; M. Weger
planes. The method for calculating the Greens functions takes into account the spatial variation of the order parameter and superconducting flow for the Abrikosov vortex lattice. For in-plane magnetic field we obtain variations of the in-plane
Physica C-superconductivity and Its Applications | 1988
L. Tewordt; D. Fay; Th. Wölkhausen
\ensuremath{\kappa}
Solid State Communications | 1978
J. Appel; D. Fay
with twofold symmetry as a function of rotation angle where the minima and maxima occur for field directions parallel and perpendicular to the heat flow. The amplitude of the variation decreases with increasing impurity scattering and temperature. At higher temperatures the minima and maxima of the variation are interchanged. Since the results for vertical and horizontal line nodes are almost the same we cannot say which of the two pairing models is more compatible with recent measurements of