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Experimental demonstration of a reconfigurable acoustic second-order topological insulator using condensed soda cans array

机译:使用缩合苏打罐阵列的可重构声学二阶拓扑绝缘体的实验证明

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摘要

Traditional topological insulators support the topologically protected boundary states that are one dimension lower than the system itself. Recently,higher-order topological insulators have received increasing attention in the field of acoustic wave manipulation due to their unique bulk-boundary correspondence principle,hosting both gapped edge states and in-gap corner states simultaneously. However,for most of the topological acoustic systems,the lack of reconfigurability and the inevitable outer trivial regions with considerable thickness restrict the potential applications of acoustic topological insulators. Here,we experimentally demonstrate a reconfigurable condensed acoustic second-order topological insulator in free space by using subwavelength soda cans whose side length is significantly reduced to 1.89 times of the corresponding wavelength. The topological nontrivial phase is introduced through tunably modulating the interval between cans. Without the typically required outer trivial regions,we observe the topological corner states at the corner of the finite structures in both simulations and experiments. Furthermore,the robustness against the defects induced by dislocations and deformations is discussed. We foresee that the proposal may facilitate the application potentials of topological acoustics in low-frequency sound manipulations.
机译:传统的拓扑绝缘体支持拓扑保护的边界状态,这些边界状态是一个比系统本身低的维度。最近,由于其独特的散对对应原理,高阶拓扑绝缘体由于其独特的散界对应原理而导致声波操作领域的越来越关注,同时托管两个覆盖的边缘状态和间隙拐角状态。然而,对于大多数拓扑声学系统,具有相当大的厚度的可重新配置性和不可避免的外部微观区域限制了声学拓扑绝缘体的潜在应用。这里,我们通过使用副长度显着降低到相应波长的1.89倍的亚波长苏打汽油罐来实验地证明可重新配置的冷凝声学二阶绝缘体。通过可调地调节罐之间的间隔来引入拓扑非竞争阶段。没有通常需要的外部琐碎区域,我们在模拟和实验中观察有限结构拐角处的拓扑角状态。此外,讨论了对脱位和变形引起的缺陷的鲁棒性。我们预见,该提案可以促进低频声音操纵中拓扑声学的应用潜力。

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  • 来源
    《Applied Physics Letters》 |2021年第20期|203501.1-203501.6|共6页
  • 作者单位

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

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

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

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

    Department of Physics MOE Key Laboratory of Modern Acoustics 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;

    Department of Physics MOE Key Laboratory of Modern Acoustics 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;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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