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Dissipation in the superconducting state of κ−(BEDT−TTF)2Cu(NCS)2

Liang Yin, Moon-Sun Nam, James G. Analytis, Stephen J. Blundell, Arzhang Ardavan, John A. Schlueter, Takahiko Sasaki

DOI 10.1103/PhysRevB.76.014506 · Physical Review B

T1

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Abstract

We have studied the interlayer resistivity of the prototypical quasi-two-dimensional organic superconductor κ−(BEDT−TTF)2Cu(NCS)2 as a function of temperature, current, and magnetic field, within the superconducting state. We find a region of nonzero resistivity whose properties are strongly dependent on magnetic field and current density. There is a crossover to non-Ohmic conduction below a temperature that coincides with the two-dimensional vortex solid–vortex liquid transition. We interpret the behavior in terms of a model of current- and thermally driven phase slips caused by the diffusive motion of the pancake vortices which are weakly coupled in adjacent layers, giving rise to a finite interlayer resistance.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
κ-(BEDT-TTF)2Cu(NCS)2

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10Pressure unresolvedmidpoint
κ-(BEDT-TTF)2Cu(NCS)2

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

10Pressure unresolvedonset
κ-(BEDT-TTF)4Hg2.89Br8

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown
α-(BEDT-TTF)2NH4Hg(SCN)4

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown

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