We report heat-capacity measurements on untwinned YBa2Cu307-a single crystals in magnetic fields //<7T, for both Hllc and HJLc. Adding Gaussian fluctuations to a BCS-like step, we obtain a fit for //-0, T~T C that is consistent with a 3D, two-component order parameter in the strong-coupling limit. However, the H^O data are inconsistent with this approach. A finite-size-scaling analysis, assuming critical behavior and an //-dependent length, satisfactorily describes the data.
We present an experimental study of the effects of oxidation on the magnetic and crystal structures of exchange biased epsilon-Co/CoO core-shell nanoparticles. Transmission electron microscopy measurements reveal that oxidation creates a Co-CoO interface which is highly directional and epitaxial in quality. Neutron diffraction measurements find that below a Néel temperature TN of approximately 235 K the magnetization of the CoO shell is modulated by two wave vectors, q1=(1/2 1/2 1/2)2pi/a and q2=(100)2pi/a. Oxidation affects the q1 component of the magnetization very little, but hugely enhances the q2 component, resulting in the magnetic decompensation of the core-shell interface. We propose that the large exchange bias effect results from the highly ordered interface between the Co core and CoO shell, and from enhanced core-shell coupling by the uncompensated interface moment.
Inderhees etal Reply:In our Letter, we reported on measurements of the specific heat of two single crystals of YBa2Cu307-<5 near the superconducting transition temperature T c . We observed a deviation from the usual mean-field discontinuity, which we attributed to Gaussian thermodynamic fluctuations. For a conventional superconductor, the amplitude ratio C + IC~ would be expected to be that of an O(n) Ginzburg-Landau theory, with «=2. In this case, the amplitude ratio is a universal number, 2 allowing us to test the hypothesis that YBa2Cu3C>7-5 is a conventional superconductor. Analyzing our data as if they corresponded to an OOi) model, we found that 5.6
Gaussian fluctuations have been observed in the specific heat of two single crystals of YBa2Cu3C>7-$. Deviations from a BCS-type step are well accounted for by 3D Gaussian fluctuations whose amplitude ratio, in the cleaner sample, implies that the number of order-parameter components is 7 ± 2. This result is inconsistent with an 0(2) Ginzburg-Landau theory.
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