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Fluctuation effects and mixed-state properties of the layered organic superconductors κ-(BEDT-TTF)2Cu(NCS)2 and κ-(BEDT-TTF)2Cu[N(CN)2]Br

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Lang, M., Steglich, F., Toyota, N., & Sasaki, T. (1994). Fluctuation effects and mixed-state properties of the layered organic superconductors κ-(BEDT-TTF)2Cu(NCS)2 and κ-(BEDT-TTF)2Cu[N(CN)2]Br. Physical Review B, 49(21), 15227-15234. doi:10.1103/PhysRevB.49.15227.


Cite as: http://hdl.handle.net/11858/00-001M-0000-0019-DDD4-E
Abstract
We report on dc-magnetization measurements on high-quality single crystals of the organic superconductors kappa-(BEDT-TTF)2 Cu(NCS)2 and kappa-(BEDT-TTF)2Cu[N(CN)2]Br for fields parallel and perpendicular to the conducting planes. For H perpendicular to the planes, we find clear indications for strong superconducting fluctuations, i.e., a pronounced rounding of the transition with increasing field and field-induced diamagnetism above T(c). Careful experiments near T(c) reveal the existence of a field-independent magnetization at M*(T*,H) for H less-than-or-equal-to 10 kOe. The anisotropy of superconducting parameters such as the upper critical field and coherence length, along with a scaling form of the high-field magnetization data demonstrate the highly anisotropic character for the present superconductors. Over an extended range in the H-T plane the mixed-state properties are governed by an entirely reversible vortex motion. The lower boundary of this range, the so-called irreversibility line, is found to be anisotropic and, for H perpendicular to the planes, to follow an exponential T dependence. Cooling below the irreversibility line is accompanied by the occurrence of magnetic relaxation effects, indicating a metastable vortex state.