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arXiv 2303.08321cond-mat.mes-hall

拓扑约瑟夫森结构中的磁化动力学与派尔斯不稳定性

Magnetization Dynamics and Peierls Instability in Topological Josephson Structures

Adrian Reich, Erez Berg, Jörg Schmalian, Alexander Shnirman

AI总结:

该研究针对夹铁磁条带的长型拓扑约瑟夫森结,揭示磁振子介导的马约拉纳费米子长程非局域相互作用可引发$\text{Z}_2$对称破缺,明确非局域性的稳定作用,并分析了孤子与关联长度特性。

摘要:

我们研究了两个超导体之间夹有铁磁条带的长型拓扑约瑟夫森结。低能理论显示,手性马约拉纳费米子之间存在时间和空间上的非局域相互作用,该相互作用由铁磁体中的磁振子激发介导。虽然短程相互作用经幂次计数证明是无关的,但我们表明,足够强的长程相互作用可能引发$\boldsymbol{\rm \text{Z}}_2$对称性破缺。这种自发破缺会导致磁化强度沿垂直于马约拉纳费米子传播的方向倾斜,并打开费米能隙(马约拉纳质量)。这一现象与公度弗罗利希模型中的派尔斯不稳定性类似,反映了马约拉纳模式与磁化动力学之间的非平凡相互作用。\n在高斯涨落分析框架内,我们估算了相互作用的时间和空间非局域性临界值;尽管模型是有效一维的,当非局域性超过该临界值时,对称性破缺在零温下是稳定的。我们得出结论:非局域性,即磁化强度在空间和时间上的刚度,能够稳定对称性破缺。在稳定区域内,我们预计电流-相位关系会出现实验可观测的不连续跳变。在非零温度下,与一维伊辛模型中的常见情况一致,长程有序会被孤子激发破坏,而我们研究体系中的每个孤子都携带一个马约拉纳零能模。为了估算关联长度,我们采用自洽平均场方法对孤子进行了研究。

英文摘要:

We study a long topological Josephson junction with a ferromagnetic strip between two superconductors. The low-energy theory exhibits a non-local in time and space interaction between chiral Majorana fermions, mediated by the magnonic excitations in the ferromagnet. While short ranged interactions turn out to be irrelevant by power counting, we show that sufficiently strong and long-ranged interactions may induce a $\mathbb{Z}_2$-symmetry breaking. This spontaneous breaking leads to a tilting of the magnetization perpendicular to the Majorana propagation direction and the opening of a fermionic gap (Majorana mass). It is analogous to the Peierls instability in the commensurate Fröhlich model and reflects the nontrivial interplay between Majorana modes and magnetization dynamics. Within a Gaussian fluctuation analysis, we estimate critical values for the temporal and spatial non-locality of the interaction, beyond which the symmetry breaking is stable at zero temperature -- despite the effective one-dimensionality of the model. We conclude that non-locality, i.e., the stiffness of the magnetization in space and time, stabilizes the symmetry breaking. In the stabilized regime, we expect the current-phase relation to exhibit an experimentally accessible discontinuous jump. At nonzero temperatures, as usual in the 1D Ising model, the long-range order is destroyed by solitonic excitations, which in our case carry each a Majorana zero mode. In order to estimate the correlation length, we investigate the solitons within a self-consistent mean-field approach.

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