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Spin-polarized Josephson current in superconductor/ferromagnet/superconductor junctions with inhomogeneous magnetization

机译:超导体/铁磁体/超导体结中的自旋极化约瑟夫森电流,磁化不均匀

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摘要

We study numerically the properties of spin transport and charge transport in a current-biased nanoscale diffusive superconductor/ferromagnet/superconductor junction when the magnetization texture is nonuniform. Specifically, we incorporate the presence of a Bloch/Neel domain walls and conical ferromagnetism, including the role of spin-active interfaces. The superconducting leads are assumed to be of the conventional s-wave type. In particular, we investigate how the 0-π transition is influenced by the inhomogeneous magnetization texture and focus on the particular case where the charge current vanishes while the spin current is nonzero. In the case of a Bloch/Neel domain wall, the spin current can be seen only for one component of the spin polarization, whereas in the case of conical ferromagnetism the spin current has the three components. This is in contrast to a scenario with a homogeneous exchange field, where the spin current vanishes completely. We explain all of these results in terms of the interplay between the triplet anomalous Green's function induced in the ferromagnetic region and the local direction of the magnetization vector in the ferromagnet. Interestingly, we find that the spin current exhibits discontinuous jumps at the 0-π transition points of the critical charge current. This is seen both in the presence of a domain wall and for conical ferromagnetism. We explain this result in terms of the different symmetry obeyed by the current-phase relation when comparing the charge and spin currents. Specifically, we find that whereas the charge current obeys the well-known relation I_c(φ) = -I_c(-φ), the spin current satisfies I_s(φ)=I_s(-φ), where φ is the superconducting phase difference.
机译:我们数值研究了当磁化织构不均匀时,在电流偏置的纳米级扩散超导体/铁磁体/超导体结中的自旋输运和电荷输运的特性。具体来说,我们结合了Bloch / Neel畴壁和锥形铁磁性的存在,包括自旋-活性界面的作用。假定超导引线是常规的s波型。特别地,我们研究了不均匀磁化纹理如何影响0-π跃迁,并着重于自旋电流为非零而电荷电流消失的特定情况。在Bloch / Neel畴壁的情况下,仅对于自旋极化的一个分量可以看到自旋电流,而在锥形铁磁的情况下,自旋电流具有三个分量。这与具有均匀交换场的情况相反,在这种情况下,自旋电流完全消失。我们根据铁磁区域中感应的三重态异常格林函数与铁磁体中磁化矢量的局部方向之间的相互作用来解释所有这些结果。有趣的是,我们发现自旋电流在临界充电电流的0-π过渡点处表现出不连续的跳跃。在存在畴壁和锥形铁磁性的情况下都可以看到这一点。当比较充电电流和自旋电流时,我们根据电流-相位关系遵循的不同对称性来解释此结果。具体地说,我们发现,尽管充电电流遵循众所周知的关系I_c(φ)= -I_c(-φ),但自旋电流满足I_s(φ)= I_s(-φ),其中φ是超导相位差。

著录项

  • 来源
    《Physical review 》 |2010年第1期| 014512.1-014512.9| 共9页
  • 作者单位

    Department of Physics, Faculty of Sciences, University of Isfahan, Hezar Jerib Avenue, Isfahan 81746-73441, Iran;

    Department of Physics, Norwegian University of Science and Technology, N-749I Trondheim, Norway;

    Department of Physics, Faculty of Sciences, University of Isfahan, Hezar Jerib Avenue, Isfahan 81746-73441, Iran;

    Department of Applied Physics, University of Tokyo, Tokyo 113-8656, Japan;

    Department of Physics, Norwegian University of Science and Technology, N-749I Trondheim, Norway;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    mesoscopic and nanoscale systems;

    机译:介观和纳米系统;

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