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超导/铁磁体界面处磁依赖无隙奇频态的特征

Signature of magnetic-dependent gapless odd frequency states at superconductor/ferromagnet interfaces.

作者信息

Di Bernardo A, Diesch S, Gu Y, Linder J, Divitini G, Ducati C, Scheer E, Blamire M G, Robinson J W A

机构信息

Department of Material Science and Metallurgy, University of Cambridge, 27 Charles Babbage Road, Cambridge CB3 0FS, UK.

Department of Physics, University of Konstanz, Konstanz 78457, Germany.

出版信息

Nat Commun. 2015 Sep 2;6:8053. doi: 10.1038/ncomms9053.

Abstract

The theory of superconductivity developed by Bardeen, Cooper and Schrieffer (BCS) explains the stabilization of electron pairs into a spin-singlet, even frequency, state by the formation of an energy gap within which the density of states is zero. At a superconductor interface with an inhomogeneous ferromagnet, a gapless odd frequency superconducting state is predicted, in which the Cooper pairs are in a spin-triplet state. Although indirect evidence for such a state has been obtained, the gap structure and pairing symmetry have not so far been determined. Here we report scanning tunnelling spectroscopy of Nb superconducting films proximity coupled to epitaxial Ho. These measurements reveal pronounced changes to the Nb subgap superconducting density of states on driving the Ho through a metamagnetic transition from a helical antiferromagnetic to a homogeneous ferromagnetic state for which a BCS-like gap is recovered. The results prove odd frequency spin-triplet superconductivity at superconductor/inhomogeneous magnet interfaces.

摘要

由巴丁、库珀和施里弗(BCS)提出的超导理论解释了电子对如何通过形成能隙而稳定成自旋单重态、偶数频率态,在此能隙内态密度为零。在与非均匀铁磁体的超导体界面处,预测会出现无隙奇数频率超导态,其中库珀对处于自旋三重态。尽管已获得这种状态的间接证据,但迄今为止,能隙结构和配对对称性尚未确定。在此,我们报告了与外延钬邻近耦合的铌超导薄膜的扫描隧道谱。这些测量揭示了在驱动钬通过从螺旋反铁磁体到均匀铁磁体的亚磁转变(此时恢复了类似BCS的能隙)时,铌亚能隙超导态密度发生了显著变化。结果证明了在超导体/非均匀磁体界面处存在奇数频率自旋三重态超导性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7ead/4569701/3ba3d95a6d48/ncomms9053-f1.jpg

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