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广义耗散马约拉纳线的拓扑态

Topological states of generalized dissipative Majorana wires.

作者信息

Hosseinifar Farokhnaz, Moghaddam Ali G

机构信息

Department of Physics, Institute for Advanced Studies in Basic Sciences (IASBS), Zanjan 45137-66731, Iran.

Research Center for Basic Sciences & Modern Technologies (RBST), Institute for Advanced Studies in Basic Science (IASBS), Zanjan 45137-66731, Iran.

出版信息

J Phys Condens Matter. 2022 Nov 9;51(2). doi: 10.1088/1361-648X/ac9ef7.

DOI:10.1088/1361-648X/ac9ef7
PMID:36317366
Abstract

We study the generalized one-dimensional (1D) quantum dissipative models corresponding to a Majorana wire which can possess more than one Majorana bound state at each end. The system consists of a 1D fermionic open quantum system whose dynamics is governed by a quadratic Lindblad equation. Using the adjoint Lindblad equation for the fermionic two-point correlations, we find the gaps in the damping and purity spectra of a generic 1D model. Then, using the symmetry-based classification, we show that a winding number as the topological invariant can be defined which distinguishes different steady states of the system in the presence of damping and purity gaps. Then we focus on certain models with different Lindblad quantum jump terms and explore their phase diagrams by calculating the damping and the purity gaps as well as the winding number. In particular, we show that by inclusion of quantum jumps between next-nearest-neighbor sites, higher winding numbers and equivalently more Majorana bound states can be achieved. Also, by introducing imbalanced couplings we can switch between states with negative and positive winding numbers. Finally, we should mention that since our formulation is based on the fermionic correlations rather than the Majorana operators, it can be easily extended to the dissipative topological phases belonging to other symmetry classes.

摘要

我们研究了与马约拉纳线相对应的广义一维(1D)量子耗散模型,该模型在每一端可能拥有不止一个马约拉纳束缚态。系统由一个一维费米子开放量子系统组成,其动力学由二次林德布拉德方程支配。利用费米子两点关联的伴随林德布拉德方程,我们找到了一般一维模型的阻尼和纯度谱中的能隙。然后,通过基于对称性的分类,我们表明可以定义一个作为拓扑不变量的缠绕数,它在存在阻尼和纯度能隙的情况下区分系统的不同稳态。接着,我们关注具有不同林德布拉德量子跃迁项的某些模型,并通过计算阻尼和纯度能隙以及缠绕数来探索它们的相图。特别地,我们表明通过包含次近邻格点之间的量子跃迁,可以实现更高的缠绕数,等效地也可以实现更多的马约拉纳束缚态。此外,通过引入不平衡耦合,我们可以在具有负缠绕数和正缠绕数的状态之间切换。最后,我们应该提到,由于我们的公式基于费米子关联而非马约拉纳算符,它可以很容易地扩展到属于其他对称类别的耗散拓扑相。

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