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首页> 外文期刊>Journal of Physics. Condensed Matter >Andreev and Majorana bound states in single and double quantum dot structures
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Andreev and Majorana bound states in single and double quantum dot structures

机译:单和双量子点结构中的Andreev和Majorana束缚态

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We present a numerical study of the emergence of Majorana and Andreev bound states in a system composed of two quantum dots, one of which is coupled to a conventional superconductor, SC1, and the other connects to a topological superconductor, SC2. By controlling the interdot coupling we can drive the system from two single (uncoupled) quantum dots to double (coupled) dot system configurations. We employ a recursive Green's function technique that provides us with numerically exact results for the local density of states of the system. We first show that in the uncoupled dot configuration (single dot behavior) the Majorana and the Andreev bound states appear in an individual dot in two completely distinct regimes. Therefore, they cannot coexist in the single quantum dot system. We then study the coexistence of these states in the coupled double dot configuration. In this situation we show that in the trivial phase of SC2, the Andreev states are bound to an individual quantum dot in the atomic regime (weak interdot coupling) or extended over the entire molecule in the molecular regime (strong interdot coupling). More interesting features are actually seen in the topological phase of SC2. In this case, in the atomic limit, the Andreev states appear bound to one of the quantum dots while a Majorana zero mode appears in the other one. In the molecular regime, on the other hand, the Andreev bound states take over the entire molecule while the Majorana state remains always bound to one of the quantum dots.
机译:我们对由两个量子点组成的系统中Majorana和Andreev束缚态的出现进行了数值研究,其中一个量子点与常规超导体SC1耦合,另一个与拓扑超导体SC2连接。通过控制点间耦合,我们可以将系统从两个单(未耦合)量子点驱动到双(耦合)点系统配置。我们采用递归格林函数技术,为我们提供系统状态局部密度的精确数值结果。我们首先表明,在非耦合点配置(单点行为)中,马约拉那和安德列夫的束缚态出现在两个完全不同的状态下的单个点中。因此,它们不能在单个量子点系统中共存。然后,我们研究在耦合双点配置中这些状态的共存。在这种情况下,我们表明在SC2的琐碎阶段中,Andreev状态在原子状态下绑定到单个量子点(弱的点间耦合)或在分子状态下扩展到整个分子上(强的点间耦合)。实际上,在SC2的拓扑阶段中可以看到更多有趣的功能。在这种情况下,在原子极限内,安德列夫态似乎束缚于其中一个量子点,而马约拉那零模出现在另一量子点上。另一方面,在分子体系中,安德列夫键合态占据了整个分子,而马约拉纳态始终保持与一个量子点结合。

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