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Enhancement of critical current density in superconducting/magnetic multi-layers with slow magnetic relaxation dynamics and large magnetic susceptibility

机译:提高超导/磁场中的临界电流密度   具有慢磁弛豫动力学和大磁性的多层   感受性

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摘要

We propose to use superconductor-magnet multi-layer structure to achieve highcritical current density by invoking polaronic mechanism of pinning. Themagnetic layers should have large magnetic susceptibility to enhance thecoupling between vortices and magnetization in magnetic layers. The relaxationof the magnetization should be slow. When the velocity of vortices is low, theyare dressed by nonuniform magnetization and move as polarons. In this case, theviscosity of vortices proportional to the magnetic relaxation time is enhancedsignificantly. As velocity increases, the polarons dissociate and the viscositydrops to the usual Bardeen-Stephen one, resulting in a jump in the I-V curve.Experimentally the jump shows up as a depinning transition and thecorresponding current at the jump is the depinning current. For Nb and propermagnet multi-layer structure, we estimate the critical current density $J_c\sim10^{9}\ \rm{A/m^2}$ at magnetic field $B\approx 1$ T.
机译:我们建议使用超导体-磁体多层结构,通过激发钉扎的极化子机制来实现高临界电流密度。磁性层应具有较大的磁化率,以增强磁性层中涡旋和磁化之间的耦合。磁化的松弛应该是缓慢的。当旋涡的速度较低时,它们会被不均匀的磁化所包裹,并以极化子的形式运动。在这种情况下,与磁弛豫时间成正比的涡旋粘度显着提高。随着速度的增加,极化子解离,粘度下降至通常的Bardeen-Stephen惯性,导致I-V曲线跳变。实验上该跳变显示为去钉化转变,相应的电流为去钉化电流。对于Nb和适当的磁体多层结构,我们估计在磁场$ B \大约1 $ T时的临界电流密度$ J_c \ sim10 ^ {9} \\ rm {A / m ^ 2} $。

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  • 年度 2012
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  • 正文语种 {"code":"en","name":"English","id":9}
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