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Superconductivity and vortex pinning in Fe <sub>1.04</sub> Te <sub>0.60</sub> Se <sub>0.40</sub> single crystal
22
Citations
12
References
2010
Year
Superconducting MaterialMagnetic PropertiesEngineeringBismuth-based SuperconductorsMagnetic MaterialsMagnetic Hysteresis LoopMagnetismSuperconductivityQuantum MaterialsHigh Tc SuperconductorsSuperconducting DevicesMaterials ScienceHigh-tc SuperconductivityPhysicsCrystalline DefectsδTc PinningIron-based SuperconductorsVortex PinningCrystallographyTransition Metal ChalcogenidesFerromagnetismHigh-temperature SuperconductivityNatural SciencesApplied PhysicsCondensed Matter PhysicsAfe2as2 Superconductors
Measurements of specific heat, resistivity, and magnetic hysteresis loop were performed on high-quality Fe1.04Te0.60Se0.40 single crystal. The exponential decay of the specific heat of the sample can be well described by the BCS-weak coupling theory. The resistive upper critical fields Hc2 were extracted with the zero-resistance criteria. The slopes dHc2ab /dT and dHc2c /dT collected from the existing data in the iron chalcogenide family are roughly scaled by the relation dHc2 /dT∝Tc for both H∥c and H∥ab configurations, which can be interpreted in terms of a pair-breaking effect. Comparing the AFe2As2 superconductors, the second magnetization peak observed in the magnetic hysteresis loops for H∥c is strongly broadened for the Fe1.04Te0.60Se0.40 single crystal. We demonstrate that the δTc pinning associated with spatial fluctuations of the transition temperatures gives rise to the broadening of the second peak.
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