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Critical temperature oscillations in superconductor-ferromagnet trilayers.

机译:超导体-铁磁体三层中的临界温度振荡。

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摘要

The interplay between superconductivity (S) and ferromagnetism (F) results in many interesting physical effects. Strong suppression of superconductivity by magnetic impurities was discovered many years ago. Investigation of this phenomena evolved into the understanding of gapless superconductive state and subsequent discovery of the mid-gap localized electronic states. On the other hand, uniform material with both superconducting and magnetic interactions was predicted to develop a periodic Fulde-Ferrel-Larkin-Ovchinnikov state.; Advances in metal film growth lead to the emergence of hybrid superconductor-ferromagnet multilayer structures - the simplest intermediates between a single impurity in a superconducting matrix and uniform magnetic superconductors. The interplay between magnetism and superconductivity happens near the F/S boundaries but becomes important to their finite concentration. Even the simplest trilayer hybrid thin film structures exhibit novel properties. An example is the S/F/S Josephson junction, which can be put into a state where the phases of the adjacent superconductors differ by pi. Following the experimental observation of this "pi-state", the field of F/S multilayers experienced a surge of interest.; In the present thesis the F/S/F trilayers are investigated. Superconducting critical temperature of such structures was predicted to depend on the mutual orientation of the F-layer magnetizations. This result was recently confirmed experimentally in trilayers composed of sufficiently disordered films that permit analysis in the framework of Usadel equations. Experiments were in qualitative agreement with the theory, however the approximations employed in the literature to solve Usadel equations were clearly invalid in the parameter range of experimental interest. To get a quantitative description of the effect, a numerical method was developed to analyze the F/S/F structures. The method was generalized for the case non-symmetric structures with different F-layers and F/S boundary properties. Our numeric results show that experiments cannot be described by the theory of symmetric structures, but can be accounted for by introducing asymmetry in the F/S boundary transparencies. We then suggest how such asymmetry of boundary parameters can be independently tested. The dependence of critical temperature on the magnetic configuration is discussed in terms of superconductor spin-triplet order parameter arising at the F/S boundaries.
机译:超导(S)和铁磁性(F)之间的相互作用导致许多有趣的物理效应。多年前发现了磁性杂质对超导性的强烈抑制。对这种现象的研究演变成对无间隙超导态的理解,以及随后对中间隙局部电子态的发现。另一方面,预计具有超导和磁相互作用的均匀材料将形成周期性的Fulde-Ferrel-Larkin-Ovchinnikov态。金属膜生长的进步导致出现了混合超导体-铁磁体多层结构-超导基质中单一杂质与均匀磁性超导体之间的最简单中间体。磁和超导之间的相互作用发生在F / S边界附近,但对它们的有限集中度很重要。即使是最简单的三层混合薄膜结构,也具有新颖的性能。一个示例是S / F / S约瑟夫森结,可以将其置于相邻超导体的相位相差π的状态。在对这种“π态”进行实验观察之后,F / S多层膜领域引起了人们的关注。在本文中,研究了F / S / F三层。预测这种结构的超导临界温度取决于F层磁化的相互取向。最近,在由充分无序的膜组成的三层膜中实验证实了这一结果,从而可以在Usadel方程的框架内进行分析。实验与该理论在质上是一致的,但是文献中用来解决Usadel方程的近似在实验兴趣的参数范围内显然是无效的。为了定量描述这种影响,开发了一种数值方法来分析F / S / F结构。该方法适用于具有不同F层和F / S边界特性的非对称结构的情况。我们的数值结果表明,实验不能用对称结构的理论来描述,但可以通过在F / S边界透明胶片中引入不对称来解决。然后,我们建议如何独立测试边界参数的这种不对称性。根据在F / S边界出现的超导体自旋三重态阶跃参数讨论了临界温度对磁性构型的依赖性。

著录项

  • 作者

    Litvak, Leonid.;

  • 作者单位

    Stanford University.;

  • 授予单位 Stanford University.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 2006
  • 页码 94 p.
  • 总页数 94
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 O49;
  • 关键词

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