One Majorana doublet can be realized at each end of thetime-reversal-invariant Majorana nanowires. We investigate the Josephson effectin the Majorana-doublet-presented junction modified by different inter-doubletcoupling manners. It is found that when the Majorana doublets couple indirectlyvia a non-magnetic quantum dot, only the normal Josephson effects occur, andthe fermion parity in the system just affects the current direction andamplitude. However, in the odd-parity case, applying finite magnetic field onthe quantum dot can induce the appearance of the fractional Josephson effect.Next, when the direct and indirect couplings between the Majorana doubletscoexist, no fractional Josephson effect takes place, regardless of finitemagnetic field on the quantum dot. Instead, the $\pi$-period current has anopportunity to appear in some special cases. All the results are clarified byanalyzing the influence of the fermion occupation in the quantum dot on theparity conservation in the whole system. We ascertain that this work will behelpful for describing the dot-assisted Josephson effect between the Majoranadoublets.
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机译:时变不变的Majorana纳米线的每一端都可以实现一个Majorana双峰。我们研究了约瑟夫森效应在不同的双峰间耦合方式修饰的马约拉纳峰-双峰呈现的交界处。研究发现,当马约拉纳峰通过非磁性量子点间接耦合时,只有正常的约瑟夫森效应发生,系统中的费米子奇偶性仅影响电流的方向和幅度。但是,在奇偶校验情况下,在量子点上施加有限的磁场会导致分数约瑟夫森效应的出现。接下来,当马约拉那双壁垒之间存在直接和间接耦合时,无论有限磁场如何都不会发生分数约瑟夫森效应。在量子点上相反,在某些特殊情况下,$ \ pi $周期电流没有机会出现。通过分析量子点中的费米子占据对整个系统奇偶性守恒的影响,可以澄清所有结果。我们确定这项工作将有助于描述Majoranadoublets之间的点辅助约瑟夫森效应。
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