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arXiv 1403.0844cond-mat.supr-con
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隧道二极管振荡器测量FeTe0:5Se 0:5的上临界磁场

Tunnel diode oscillator measurements of the upper critical magnetic field of FeTe0:5Se0:5

Alain Audouard, Loïc Drigo, Fabienne Duc, Xavier Fabrèges, Ludovic Bosseaux, Pierre Toulemonde

摘要:

在磁场高达55 T、温度低至1.6 K的条件下,用隧道二极管双极型超导体测量了FeTe_(0.5)Se_(0.5)(Tc = 14.5 K)的上临界磁场(Hc_2)随温度的变化关系。Werthamer-Helfand-Hohenberg模型解释了平行(H)和平行(H)施加的磁场的数据||ab)和垂直(H|| c)到铁导电平面,符合单带超导性。而对于H,泡利对破缺可以忽略不计,||c,证明了H的泡利贡献||ab,Maki参数α = 1.4,对应于Pauli场HP = 79 T。结果,在Tc(γ = 1.6)下已经相当小的Hc 2各向异性(= Habc 2/Hcc 2)随着温度降低而进一步减小,并且在液氦温度下变得小于1。

英文摘要:

Temperature dependence of the upper critical magnetic field (Hc2) of single crystalline FeTe0.5Se0.5 (Tc = 14.5 K) have been determined by tunnel diode oscillator-based measurements in magnetic fields of up to 55 T and temperatures down to 1.6 K. The Werthamer-Helfand-Hohenberg model accounts for the data for magnetic field applied both parallel (H || ab) and perpendicular (H || c) to the iron conducting plane, in line with a single band superconductivity. Whereas Pauli pair breaking is negligible for H || c, Pauli contribution is evidenced for H || ab with Maki parameter alpha= 1.4, corresponding to Pauli field HP = 79 T. As a result, the Hc2 anisotropy (= Habc2 /Hcc2) which is already rather small at Tc (gamma = 1.6) further decreases as the temperature decreases and becomes smaller than 1 at liquid helium temperatures.

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