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Effects of magnetic anisotropy on the subgap excitations induced by quantum impurities in a superconducting host

机译:磁各向异性对超导主体中量子杂质引起的亚能隙激发的影响

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摘要

We study the magnetic anisotropy effects on the localized subgap excitations induced by quantum impurities coupled to a superconducting host. We establish the ground-state phase diagrams for single-channel and two-channel high-spin Kondo impurities; they unveil surprising complexity that results from the (multistage) Kondo screening in competition with the superconducting correlations and the magnetic anisotropy splitting of the spin multiplets. We discuss the possibility of detecting the Zeeman splitting of the subgap states, which would provide an interesting spectroscopic tool for studying the magnetism on the single-atom level. We also study the problem of two impurities coupled by the Heisenberg exchange interaction, and we follow the evolution of the subgap states for both antiferromagnetic and ferromagnetic coupling. For sufficiently strong antiferromagnetic coupling, the impurities bind into a singlet state that is nonmagnetic, thus the subgap states move to the edge of the gap and can no longer be discerned. For ferromagnetic coupling, some excited states remain present inside the gap.
机译:我们研究了耦合到超导主体的量子杂质对局部亚隙激发的磁各向异性效应。我们建立了单通道和两通道高自旋近藤杂质的基态相图;他们揭示了(多级)近藤筛选与超导相关性和自旋多重峰的磁各向异性分裂所产生的惊人复杂性。我们讨论了检测子能隙态的塞曼分裂的可能性,这将为研究单原子级的磁性提供一个有趣的光谱工具。我们还研究了通过Heisenberg交换相互作用耦合的两种杂质的问题,并且我们跟踪了反铁磁和铁磁耦合的子能隙状态的演化。对于足够强的反铁磁耦合,杂质会结合成非磁性的单重态,因此子带隙态会移动到间隙的边缘,无法再被识别。对于铁磁耦合,一些激发态保留在间隙内部。

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