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Topolectrieal-circuit realization of a four-dimensional hexadecapole insulator

机译:TopoLieial-Circue实现四维十六峰内绝缘子

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摘要

Recently, the theory of quantized dipole polarization has been extended to account for electric multipole moments, giving rise to the discovery of multipole topological insulators (TIs). Both two-dimensional quadrupole and three-dimensional (3D) octupole TIs with robust zero-dimensional corner states have been realized in various classical systems. However, due to the intrinsic 3D limitation, the higher-dimensional multipole TIs, such as four-dimensional (4D) hexadecapole TIs, are supposed to be extremely hard to construct in real space. Here, we theoretically propose and experimentally demonstrate the realization of a classical analog of 4D hexadecapole TI based on the electric circuits in fully real space. The explicit construction of 4D hexadecapole circuits, where the connection of nodes is allowed in any desired way free from constraints of locality and dimensionality, is provided. By direct circuit simulations and impedance measurements, the in-gap corner states protected by the quantized hexadecapole moment in the 4D circuit lattices are observed and the robustness of the corner state is also demonstrated. Our work offers a pathway to study the higher-order/dimensional topological physics in real space.
机译:最近,已经扩展了量化的偶极极化理论以考虑电动多极矩,从而产生多极拓扑绝缘体(TIS)的发现。在各种古典系统中已经实现了具有鲁棒零维拐角状态的二维四极和三维(3D)Octupole TIS。然而,由于内在的3D限制,高尺寸多极TIS,例如四维(4D)十六峰TIS,应该非常难以在真实空间中构建。在这里,我们理论上提出并通过实验证明了基于完全真实空间的电路基于电路的4D Hexadapole Ti的经典模拟。提供了4D Hexadapole电路的显式结构,其中允许节点的连接以任何所需的方式从局部性和维度的约束中提供。通过直接电路模拟和阻抗测量,观察到由4D电路格子中量化的十六峰血管矩保护的间隙角状态,并且还证明了角状态的鲁棒性。我们的作品提供了一种途径,可以在真实空间中研究高阶/尺寸拓扑物理。

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  • 来源
    《Physical review.B.Condensed matter and materials physics》 |2020年第10期|100102.1-100102.7|共7页
  • 作者单位

    Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurements of Ministry of Education Beijing Key Laboratory of Nanophotonics and Ultrafine Optoelectronic Systems School of Physics Beijing Institute of Technology Beijing 100081 China;

    Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurements of Ministry of Education Beijing Key Laboratory of Nanophotonics and Ultrafine Optoelectronic Systems School of Physics Beijing Institute of Technology Beijing 100081 China;

    Beijing Key Laboratory of Millimeter Wave and Terahertz Techniques School of Information and Electronics Beijing Institute of Technology Beijing 100081 China;

    Beijing Key Laboratory of Millimeter Wave and Terahertz Techniques School of Information and Electronics Beijing Institute of Technology Beijing 100081 China;

    Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurements of Ministry of Education Beijing Key Laboratory of Nanophotonics and Ultrafine Optoelectronic Systems School of Physics Beijing Institute of Technology Beijing 100081 China;

    Beijing Key Laboratory of Millimeter Wave and Terahertz Techniques School of Information and Electronics Beijing Institute of Technology Beijing 100081 China;

    Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurements of Ministry of Education Beijing Key Laboratory of Nanophotonics and Ultrafine Optoelectronic Systems School of Physics Beijing Institute of Technology Beijing 100081 China;

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