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Topological edge states in acoustic Kagome lattices

机译:声学Kagome晶格中的拓扑边缘状态

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We demonstrate that an acoustic Kagome lattice formed by an array of interconnected resonant cavities exhibits a new class of topological states protected by C3 symmetry, and it is characterised by a topological invariant in the form of a winding number in Pauli vector space. This acoustic topological metamaterial can be considered as the two-dimensional analogue of the Su–Schrieffer–Heeger model, exhibiting a topological transition when a detuning is introduced between the inter-cell and intra-cell hopping amplitudes. The topological transition caused by such detuning is accompanied by the opening of a complete topological band gap, which may host edge states. The edge states emerge on either truncated ends of the lattice terminated by a cladding layer or at the domain walls between topologically nontrivial and trivial domains. First-principles simulations based on full-wave finite element method are used to design the lattice and confirm our analytical predictions.
机译:我们证明了由相互连接的谐振腔阵列形成的声学Kagome晶格表现出受到C3对称性保护的一类新的拓扑状态,并且其特征是在Pauli向量空间中以绕数形式的拓扑不变性。这种声学拓扑超材料可以视为Su–Schrieffer–Heeger模型的二维模拟,当在小区间和小区间跳变幅度之间引入失谐时,会表现出拓扑转变。由这种失谐引起的拓扑过渡伴随着一个完整的拓扑带隙的开放,它可能包含边缘状态。边缘状态出现在由包层终止的晶格的截断末端上,或者出现在拓扑非平凡和平凡的畴之间的畴壁上。基于全波有限元法的第一性原理模拟被用于设计晶格并确认我们的分析预测。

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