Thermodynamics of the vortex liquid in heavy ion-irradiated superconductors

Cornelis J. van der Beek; Marcin Konczykowski; Luc Fruchter; René Brusetti; Thierry Klein; Jacques Marcus; Christophe Marcenat

doi:10.1103/PhysRevB.72.214504

paper

Thermodynamics of the vortex liquid in heavy ion-irradiated superconductors

arXiv:cond-mat/0504100 · doi:10.1103/PhysRevB.72.214504

Abstract

It is shown that the large effect of heavy ion-irradiation on the thermodynamical properties of the anisotropic superconductor YBa $_{2}$ Cu $_{3}$ O $_{7 - δ}$ extends well into the superconducting fluctuation regime. The presence of the induced amorphous columnar defects shifts the specific heat maximum at the normal-to-superconducting transition. This effect is similar to that recently put into evidence in cubic K $_{x}$ Ba $_{1 - x}$ BiO $_{3}$ ( $x ≃ 0.35$ ). In both compounds, vortex pinning manifests itself as a sharp angular dependence of the \em equilibrium \rm torque. In YBa $_{2}$ Cu $_{3}$ O $_{7 - δ}$ , pinning by the defects appears at the temperature $T_{C_{p}}^{ma x}$ of the specific heat maximum, well above the magnetic irreversibility line $T_{i r r} (H)$ . In isotropic K $_{x}$ Ba $_{1 - x}$ BiO $_{3}$ , the onset of the pinning-related torque anomaly tracks the onset of the specific heat anomaly and the irreversibility line. In YBa $_{2}$ Cu $_{3}$ O $_{7 - δ}$ , fluctuations of the amplitude of the order parameter (and not vortex line wandering) are ultimately responsible for the vanishing of pinning. In K $_{x}$ Ba $_{1 - x}$ BiO $_{3}$ , vortex pinning disappears only at the superconducting-to-normal transition. The results indicate that in both compounds, the pinning energy at the ``Bose glass'' transition is large with respect to the total free energy gain in the superconducting state. By implication, the mechanism of this latter transition should be reconsidered.

arXiv comment9 pages, 9 figures, resubmitted to PRB 23-09-2005

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Cited by in corpus (1)

Thermodynamics of a Heavy Ion-Irradiated Superconductor: the Zero-Field Transition