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Spin-resolved Andreev levels and parity crossings in hybrid superconductor-semiconductor nanostructures

机译:超导体-半导体混合纳米结构中自旋分辨的安德列夫能级和奇偶穿越

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The physics and operating principles of hybrid superconductor-semiconductor devices rest ultimately on the magnetic properties of their elementary subgap excitations, usually called Andreev levels. Here we report a direct measurement of the Zeeman effect on the Andreev levels of a semiconductor quantum dot with large electron g-factor, strongly coupled to a conventional superconductor with a large critical magnetic field. This material combination allows spin degeneracy to be lifted without destroying superconductivity. We show that a spin-split Andreev level crossing the Fermi energy results in a quantum phase transition to a spin-polarized state, which implies a change in the fermionic parity of the system. This crossing manifests itself as a zero-bias conductance anomaly at finite magnetic field with properties that resemble those expected for Majorana modes in a topological superconductor. Although this resemblance is understood without evoking topological superconductivity, the observed parity transitions could be regarded as precursors of Majorana modes in the long-wire limit.
机译:混合超导体-半导体器件的物理和工作原理最终取决于其基本亚隙激发的磁性,通常称为安德列夫能级。在这里,我们报道了对具有大电子g因子的塞曼效应对具有大量电子g因子的半导体量子点的安德列夫能级的直接测量,该强耦合到具有大临界磁场的常规超导体。这种材料的结合使自旋简并性得以提升而又不破坏超导性。我们表明,穿过费米能量的自旋分裂安德烈耶夫能级导致量子相转变为自旋极化态,这暗示着系统的铁电平价发生了变化。这种交叉表现为在有限磁场下的零偏置电导异常,其性质类似于拓扑超导体中的马约拉纳模式所期望的性质。尽管在不引起拓扑超导的情况下理解了这种相似性,但是在长线范围内,观察到的奇偶性跃迁可以视为马约拉那模式的前兆。

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