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Coupled wire construction of a topological phase with chiral tricritical Ising edge modes

机译:耦合电线结构与手性三核依济阶段边缘模式的拓扑阶段

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Tricritical Ising (TCI) phase transition is known to occur in several interacting spin and Majorana fermion models and is described in terms of a supersymmetric conformal field theory (CFT) with central charge c = 7/10. The field content of this CFT is highly nontrivial and includes among its primary fields the Fibonacci anyon, making it of potential interest to strategies seeking to implement fault-tolerant topological quantum computation with non-Abelian phases of matter. In this paper we explore the possibility that a TCI CFT can occur at the edge of a gapped two-dimensional topological state as a stable phase. We discuss a possible realization of this 2D phase based on a coupled-wire construction using the Grover-Sheng-Vishwanath chain model of Majorana zero modes coupled to Ising spins which is known to undergo the TCI phase transition. From the combined analysis using mean-field theory, conformal field theory, and density matrix renormalization group (DMRG) on two- and four-leg ladders, we find that the left- and right-moving gapless TCI modes become spatially separated and reside on two opposite edges of the system, forming a precursor of the required 2D topological phase.
机译:已知三分酰基阶段(TCI)相转变发生在几种相互作用的旋转和Majorana Fermion模型中,并根据具有中央电荷C = 7/10的超对称保形场理论(CFT)来描述。该CFT的字段内容非常不动,并且在其主要领域中包括斐波纳契Anonon,使得潜在的兴趣潜在利息,寻求利用非雅中阶段实现容错拓扑量子计算。在本文中,我们探讨了TCI CFT可以发生在螺纹二维拓扑状态的边缘中的可能性,作为稳定的相位。我们讨论了基于使用耦合到依赖于旋转的Majorana零模式的耦合线结构的耦合线结构来实现这一2D相的实现。已知经历TCI相转变。通过使用平均场理论,共形场理论和密度矩阵重新定化组(DMRG)在两腿和四腿梯子上的综合分析中,我们发现左右移动的无间隙TCI模式在空间上分离并驻留系统的两个相对边缘,形成所需的2D拓扑阶段的前体。

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  • 来源
    《Physical review》 |2020年第16期|165123.1-165123.8|共8页
  • 作者单位

    Department of Physics and Astronomy & Stewart Blusson Quantum Matter Institute University of British Columbia Vancouver British Columbia V6T 1Z1 Canada;

    Department of Condensed Matter Physics Weizmann Institute of Science Rehovot 76100 Israel;

    Department of Physics and Astronomy & Stewart Blusson Quantum Matter Institute University of British Columbia Vancouver British Columbia V6T 1Z1 Canada;

    Department of Condensed Matter Physics Weizmann Institute of Science Rehovot 76100 Israel;

    Department of Physics and Astronomy & Stewart Blusson Quantum Matter Institute University of British Columbia Vancouver British Columbia V6T 1Z1 Canada;

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