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首页> 外文期刊>Physical Review. B, Condensed Matter >Andreev bound states in superconductor/ferromagnet point contact Andreev reflection spectra
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Andreev bound states in superconductor/ferromagnet point contact Andreev reflection spectra

机译:超导体/铁磁体点接触中的Andreev束缚态Andreev反射光谱

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摘要

As charge carriers traverse a single superconductor ferromagnet interface, they experience an additional spin-dependent phase angle that results in spin mixing and the formation of a bound state called the Andreev bound state. Here we explore whether point contact Andreev reflection can be used to detect the Andreev bound state and, within the limits of our experiment, we extract the resulting spin mixing angle. By examining spectra taken from La_(1.15)Sr_(1.85)Mn_2O_7-Pb junctions, together with a compilation of literature data on highly spin polarized systems, we suggest that the existence of the Andreev bound state would resolve a number of long standing controversies in the literature of Andreev reflection, as well as defining a route to quantify the strength of spin mixing at superconductor-ferromagnet interfaces. Intriguingly, we find that for high transparency junctions, the spin mixing angle appears to take a relatively narrow range of values across all the samples studied. The ferromagnets we have chosen to study share a common property in terms of their spin arrangement, and our observations may point to the importance of this property in determining the spin mixing angle under these circumstances.
机译:当电荷载流子穿过单个超导体铁磁体界面时,它们会经历一个附加的自旋相关相角,导致自旋混合并形成称为安德列夫束缚态的束缚态。在这里,我们探讨点接触Andreev反射是否可用于检测Andreev束缚状态,并在我们的实验范围内,提取所得的自旋混合角。通过检查从La_(1.15)Sr_(1.85)Mn_2O_7-Pb结处获得的光谱,以及有关高度自旋极化系统的文献数据的汇编,我们建议,Andreev束缚态的存在将解决许多长期存在的争议。 Andreev反射的文献,以及定义量化超导体-铁磁体界面上自旋混合强度的途径。有趣的是,我们发现,对于高透明结,自旋混合角在所有研究的样品中似乎取值范围相对狭窄。我们选择研究的铁磁体在自旋排列方面具有共同的特性,我们的观察结果可能表明,在这种情况下,此特性对于确定自旋混合角的重要性。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2017年第9期|094516.1-094516.8|共8页
  • 作者单位

    Physics Department, The Blackett Laboratory, Imperial College London, SW7 2AZ, United Kingdom;

    Department of Materials Science and Metallurgy, University of Cambridge, 27 Charles Babbage Road, Cambridge CB3 OFS, United Kingdom ,Faculty of Science and Technology and MESA+ Institute for Nanotechnology, University of Twente, 7500 AE Enschede, The Netherlands;

    Department of Materials Science and Metallurgy, University of Cambridge, 27 Charles Babbage Road, Cambridge CB3 OFS, United Kingdom;

    Department of Physics, Clarendon Laboratory, University of Oxford, Park Road, Oxford 0X1 3PU, United Kingdom;

    Department of Physics, American University of Sharjah, Sharjah 26666, United Arab Emirates;

    Department of Materials Science and Metallurgy, University of Cambridge, 27 Charles Babbage Road, Cambridge CB3 OFS, United Kingdom;

    Physics Department, The Blackett Laboratory, Imperial College London, SW7 2AZ, United Kingdom;

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