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Experimental demonstration of topologically protected efficient sound propagation in an acoustic waveguide network

机译:声学波导网络中拓扑保护有效声音传播的实验演示

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摘要

Acoustic topological states support sound propagation along the boundary in a one-way direction with inherentrobustness against defects and disorders, leading to the revolution of the manipulation on acoustic waves. Avariety of acoustic topological states relying on circulating fluid, chiral coupling, or temporal modulation havebeen proposed theoretically. However, experimental demonstration has so far remained a significant challenge,due to the critical limitations such as structural complexity and high losses. Here, we experimentally demonstratean acoustic anomalous Floquet topological insulator in a waveguide network. The acoustic gapless edge statescan be found in the band gap when the waveguides are strongly coupled. The scheme features simple structureand high-energy throughput, leading to the experimental demonstration of efficient and robust topologicallyprotected sound propagation along the boundary. The proposal may offer a unique, promising application fordesign of acoustic devices in acoustic guiding, switching, isolating, filtering, etc.
机译:声学拓扑状态支持沿着边界的声音传播,以单向方向具有固有的对缺陷和疾病的鲁棒性,导致操纵在声波上的操纵。一种依赖于循环液,手性耦合或时间调制的各种声学拓扑状态理论上提出。然而,到目前为止,实验示范仍然是一个重大挑战,由于结构复杂性和高损失等临界局限性。在这里,我们通过实验证明波导网络中的声学异常浮子拓扑绝缘体。声学无效边缘状态当波导强烈耦合时,可以在带隙中找到。该方案具有简单的结构和高能吞吐量,导致实验拓扑实验演示高效和稳健沿边界保护的声音传播。该提案可以提供独特的承诺申请声学引导,开关,隔离,过滤等声学装置的设计。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2017年第10期|094305.1-094305.9|共9页
  • 作者单位

    Key Laboratory of Modern Acoustics Department of Physics and Collaborative Innovation Center of Advanced Microstructures Nanjing University Nanjing 210093 China;

    Key Laboratory of Modern Acoustics Department of Physics and Collaborative Innovation Center of Advanced Microstructures Nanjing University Nanjing 210093 China;

    Key Laboratory of Modern Acoustics Department of Physics and Collaborative Innovation Center of Advanced Microstructures Nanjing University Nanjing 210093 China;

    Key Laboratory of Modern Acoustics Department of Physics and Collaborative Innovation Center of Advanced Microstructures Nanjing University Nanjing 210093 China State Key Laboratory of Acoustics Institute of Acoustics Chinese Academy of Sciences Beijing 100190 China;

    Key Laboratory of Modern Acoustics Department of Physics and Collaborative Innovation Center of Advanced Microstructures Nanjing University Nanjing 210093 China State Key Laboratory of Acoustics Institute of Acoustics Chinese Academy of Sciences Beijing 100190 China;

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