临界温度提高的超导异质结构中的界面和体超导性

G. Mazza, A. Amaricci, Massimo Capone
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引用次数: 2

摘要

我们考虑了两个耦合强度显著不同的s波超导体在弱耦合和强耦合条件下的异质结构。弱耦合超导体和强耦合超导体的临界温度相近。利用动力学平均场理论方法,我们发现,当两种超导体中的一种的单层与另一种较厚的多层交替时,所有异质结构的超导临界温度都普遍提高。两种不同的物理状态可以被识别为较大层厚度的函数:(i)一个固有的非均匀超导体,其特征是两个孤立的体超导体的特性,其中临界温度的提高仅限于界面;(ii)一个临界温度提高的体超导体延伸到整个异质结构。我们描述了这些制度之间的交叉在两个长度尺度之间的竞争与邻近效应和对相干。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Interface and bulk superconductivity in superconducting heterostructures with enhanced critical temperatures
We consider heterostructures obtained by stacking layers of two s-wave superconductors with significantly different coupling strengths, respectively in the weak- and strong-coupling regimes. The weak- and strong-coupling superconductors are chosen with similar critical temperatures for bulk systems. Using dynamical mean-field theory methods, we find an ubiquitous enhancement of the superconducting critical temperature for all the heterostructures where a single layer of one of the two superconductors is alternated with a thicker multilayer of the other. Two distinct physical regimes can be identified as a function of the thickness of the larger layer: (i) an inherently inhomogeneous superconductor characterized by the properties of the two isolated bulk superconductors where the enhancement of the critical temperature is confined to the interface and (ii) a bulk superconductor with an enhanced critical temperature extending to the whole heterostructure. We characterize the crossover between these regimes in terms of the competition between two length scales connected with the proximity effect and the pair coherence.
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