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首页> 外文期刊>Applied Physics Letters >Fluctuation of mean free path and transition temperature induced vortex pinning in (Ba,K)Fe_2As_2 superconductors
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Fluctuation of mean free path and transition temperature induced vortex pinning in (Ba,K)Fe_2As_2 superconductors

机译:(Ba,K)Fe_2As_2超导体中平均自由程和跃迁温度引起的涡旋钉扎的波动

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摘要

The vortex pinning mechanisms of Ba_(0.72)K_(0.28)Fe_2As_2 single crystal have been studied systematically as a function of temperature and magnetic field. The temperature dependence of the critical current density, J_C{T), was analysed within the collective pinning model at different magnetic fields. It was found that both the δl pinning mechanism, i.e., pinning associated with charge-carrier mean free path fluctuation, and the δT_C pinning mechanism, which is associated with spatial fluctuations of the transition temperature, coexist in the Ba_(0.72)K_(0.28)Fe_2As_2 single crystal in fields smaller than 4 T. Their contributions are strongly temperature and magnetic field dependent. At lower temperature and B ≤ 4 T, the δl pinning is the dominant mechanism, and its contributions decrease with increasing temperature. At temperatures close to the critical temperature, however, there is evidence for δT_C pinning. At magnetic fields larger than 4 T, the δl pinning mechanism is the only effect.
机译:系统地研究了Ba_(0.72)K_(0.28)Fe_2As_2单晶的涡旋钉扎机理,该机理与温度和磁场有关。在不同磁场下的集体钉扎模型中,分析了临界电流密度J_C {T)的温度依赖性。发现在Ba_(0.72)K_(0.28)中共存有δl钉扎机制,即与电荷载流子平均自由程波动相关的钉扎,和与转变温度的空间波动有关的δT_C钉扎机制。 Fe_2As_2单晶在小于4 T的场中。它们的作用与温度和磁场有关。在较低的温度和B≤4 T时,δl钉扎是主要机理,并且其贡献随着温度的升高而降低。但是,在接近临界温度的温度下,有证据表明存在δT_C钉扎现象。在大于4 T的磁场中,δl钉扎机制是唯一的作用。

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  • 来源
    《Applied Physics Letters》 |2012年第21期|p.212601.1-212601.4|共4页
  • 作者单位

    Institute for Superconducting and Electronic Materials, University of Wollongong, Wollongong, New South Wales 2522, Australia,Department of Physics, Hakim Sabzevari University, P.O. Box 397, Sabzevar, Iran;

    Institute for Superconducting and Electronic Materials, University of Wollongong, Wollongong, New South Wales 2522, Australia;

    Institute for Superconducting and Electronic Materials, University of Wollongong, Wollongong, New South Wales 2522, Australia;

    Institute for Superconducting and Electronic Materials, University of Wollongong, Wollongong, New South Wales 2522, Australia;

    Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany;

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