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交流/直流驱动的超导纳米管中的拓扑转变。

Topological transitions in ac/dc-driven superconductor nanotubes.

作者信息

Fomin Vladimir M, Rezaev Roman O, Dobrovolskiy Oleksandr V

机构信息

Institute for Integrative Nanosciences, Leibniz IFW Dresden, Helmholtzstraße 20, 01069, Dresden, Germany.

Laboratory of Physics and Engineering of Nanomaterials, Department of Theoretical Physics, Moldova State University, strada A. Mateevici 60, 2009, Chisinau, Republic of Moldova.

出版信息

Sci Rep. 2022 Jun 16;12(1):10069. doi: 10.1038/s41598-022-13543-0.

Abstract

Extending of nanostructures into the third dimension has become a major research avenue in condensed-matter physics, because of geometry- and topology-induced phenomena. In this regard, superconductor 3D nanoarchitectures feature magnetic field inhomogeneity, non-trivial topology of Meissner currents and complex dynamics of topological defects. Here, we investigate theoretically topological transitions in the dynamics of vortices and slips of the phase of the order parameter in open superconductor nanotubes under a modulated transport current. Relying upon the time-dependent Ginzburg-Landau equation, we reveal two distinct voltage regimes when (i) a dominant part of the tube is in either the normal or superconducting state and (ii) a complex interplay between vortices, phase-slip regions and screening currents determines a rich FFT voltage spectrum. Our findings unveil novel dynamical states in superconductor open nanotubes, such as paraxial and azimuthal phase-slip regions, their branching and coexistence with vortices, and allow for control of these states by superimposed dc and ac current stimuli.

摘要

由于几何和拓扑诱导现象,纳米结构向三维空间的扩展已成为凝聚态物理的一个主要研究方向。在这方面,超导体三维纳米结构具有磁场不均匀性、迈斯纳电流的非平凡拓扑结构以及拓扑缺陷的复杂动力学。在此,我们从理论上研究了在调制传输电流下开放超导体纳米管中涡旋动力学和序参量相位滑移的拓扑转变。基于含时金兹堡 - 朗道方程,我们揭示了两种不同的电压状态:(i)纳米管的主要部分处于正常态或超导态;(ii)涡旋、相位滑移区域和屏蔽电流之间的复杂相互作用决定了丰富的傅里叶变换电压谱。我们的研究结果揭示了超导体开放纳米管中的新型动力学状态,如近轴和方位角相位滑移区域、它们的分支以及与涡旋的共存,并允许通过叠加直流和交流电流刺激来控制这些状态。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5423/9203797/41028797836f/41598_2022_13543_Fig1_HTML.jpg

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