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Topologically robust sound propagation in an angular-momentum-biased graphene-like resonator lattice

机译:角动量偏置的石墨烯状谐振器晶格中的拓扑鲁棒声音传播

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摘要

Topological insulators do not allow conduction in the bulk, yet they support edge modes that travel along the boundary only in one direction, determined by the carried electron spin, with inherent robustness to defects and disorder. Topological insulators have inspired analogues in photonics and optics, in which one-way edge propagation in topologically protected two-dimensional materials is achieved breaking time-reversal symmetry with a magnetic bias. Here, we introduce the concept of topological order in classical acoustics, realizing robust topological protection and one-way edge propagation of sound in a suitably designed resonator lattice biased with angular momentum, forming the acoustic analogue of a magnetically biased graphene layer. Extending the concept of an acoustic nonreciprocal circulator based on angular-momentum bias, time-reversal symmetry is broken here using moderate rotational motion of air within each element of the lattice, which takes the role of the electron spin in determining the direction of modal edge propagation.
机译:拓扑绝缘体不允许在主体中传导,但它们支持仅在一个方向上沿边界传播的边沿模式,该方向由承载的电子自旋确定,具有固有的对缺陷和无序的鲁棒性。拓扑绝缘体启发了光子学和光学中的类似物,其中在拓扑受保护的二维材料中实现了单向边缘传播,并通过磁偏置打破了时间反转对称性。在这里,我们介绍了经典声学中的拓扑顺序的概念,在经过适当设计的谐振器晶格中以角动量偏置,从而实现了稳健的拓扑保护和声音的单边传播,从而形成了磁偏置石墨烯层的声学类似物。扩展了基于角动量偏置的声学不可逆环行器的概念,在此,使用空气在晶格的每个元素内的适度旋转运动来打破时间反转对称性,这在确定模态边的方向时起电子自旋的作用传播。

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