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在人工设计的电子近藤超晶格中控制非常规超导性。

Controlling unconventional superconductivity in artificially engineered-electron Kondo superlattices.

作者信息

Naritsuka M, Terashima T, Matsuda Y

机构信息

Department of Physics, Kyoto University, Kyoto 606-8502, Japan.

出版信息

J Phys Condens Matter. 2021 May 28;33(27). doi: 10.1088/1361-648X/abfdf2.

Abstract

Unconventional superconductivity and magnetism are intertwined on a microscopic level in a wide class of materials, including high-cuprates, iron pnictides, and heavy-fermion compounds. Interactions between superconducting electrons and bosonic fluctuations at the interface between adjacent layers in heterostructures provide a new approach to this most fundamental and hotly debated subject. We have been able to use a recent state-of-the-art molecular-beam-epitaxy technique to fabricate superlattices consisting of different heavy-fermion compounds with atomic thickness. These Kondo superlattices provide a unique opportunity to study the mutual interaction between unconventional superconductivity and magnetic order through the atomic interface. Here, we design and fabricate hybrid Kondo superlattices consisting of alternating layers of superconducting CeCoInwith-wave pairing symmetry and nonmagnetic metal YbCoInor antiferromagnetic heavy fermion metals such as CeRhInand CeIn. In these Kondo superlattices, superconducting heavy electrons are confined within the two-dimensional CeCoInblock layers and interact with neighboring nonmagnetic or magnetic layers through the interface. Superconductivity is strongly influenced by local inversion symmetry breaking at the interface in CeCoIn/YbCoInsuperlattices. The superconducting and antiferromagnetic states coexist in spatially separated layers in CeCoIn/CeRhInand CeCoIn/CeInsuperlattices, but their mutual coupling via the interface significantly modifies the superconducting and magnetic properties. The fabrication of a wide variety of hybrid superlattices paves a new way to study the relationship between unconventional superconductivity and magnetism in strongly correlated materials.

摘要

在包括高温铜酸盐、铁基氮化物和重费米子化合物在内的众多材料中,非常规超导性和磁性在微观层面相互交织。异质结构中相邻层界面处超导电子与玻色子涨落之间的相互作用为这一最基本且备受争议的课题提供了一种新方法。我们已能够利用最新的先进分子束外延技术制备由具有原子厚度的不同重费米子化合物组成的超晶格。这些近藤超晶格为通过原子界面研究非常规超导性与磁序之间的相互作用提供了独特契机。在此,我们设计并制备了由具有波配对对称性的超导CeCoIn与非磁性金属YbCoIn或反铁磁重费米子金属(如CeRhIn和CeIn)交替层组成的混合近藤超晶格。在这些近藤超晶格中,超导重电子被限制在二维CeCoIn块状层内,并通过界面与相邻的非磁性或磁性层相互作用。在CeCoIn/YbCoIn超晶格中,超导性受到界面处局部反演对称性破缺的强烈影响。在CeCoIn/CeRhIn和CeCoIn/CeIn超晶格中,超导态和反铁磁态在空间上分离的层中共存,但它们通过界面的相互耦合显著改变了超导和磁性特性。各种混合超晶格的制备为研究强关联材料中非常规超导性与磁性之间的关系开辟了一条新途径。

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