2020
DOI: 10.1103/physrevb.102.180102
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Acoustic square-root topological states

Abstract: Square-root topological states are new topological phases, whose topological property is inherited from the square of the Hamiltonian. We realize the first-order and secondorder square-root topological insulators in phononic crystals, by putting additional cavities on connecting tubes in the acoustic Su-Schrieffer-Heeger model and the honeycomb lattice, respectively. Because of the square-root procedure, the bulk gap of the squared Hamiltonian is doubled. In both two bulk gaps, the square-root topological insu… Show more

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Cited by 53 publications
(29 citation statements)
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“…Crucially, however, the cylinders were not closely spaced and the authors did not consider any topological aspects of the array; it is likely that the quality of the edge states in this system would be reduced by longerranged coupling between voids and their next-nearest-neighbours. On the other hand, Yan et al [44] studied a honeycomb-kagome array of acoustic resonators connected by narrow channels and considered the symmetry protected topology. However, in their work the width of the channels were alternated to produce a square-root topological insulator where the topology was inherited from the breathing kagome sector of the squared Hamiltonian, whereas we study the lattice with equal channel widths, which is akin to the mass-spring/tight-binding models of Mizoguchi et al [40], where the nontrivial topology is inherited from the honeycomb sector of the squared Hamiltonian.…”
Section: Mass-spring and Void-channel Modelsmentioning
confidence: 99%
“…Crucially, however, the cylinders were not closely spaced and the authors did not consider any topological aspects of the array; it is likely that the quality of the edge states in this system would be reduced by longerranged coupling between voids and their next-nearest-neighbours. On the other hand, Yan et al [44] studied a honeycomb-kagome array of acoustic resonators connected by narrow channels and considered the symmetry protected topology. However, in their work the width of the channels were alternated to produce a square-root topological insulator where the topology was inherited from the breathing kagome sector of the squared Hamiltonian, whereas we study the lattice with equal channel widths, which is akin to the mass-spring/tight-binding models of Mizoguchi et al [40], where the nontrivial topology is inherited from the honeycomb sector of the squared Hamiltonian.…”
Section: Mass-spring and Void-channel Modelsmentioning
confidence: 99%
“…After this proposal, analysis of square-root topological insulators in higher dimensions has been addressed [25][26][27][28][29][30][31][32] , which has elucidated ubiquity of the squareroot topological phases. For instance, a square-root counterpart of higher-order topological phases are reported by both theoretical 25 and experimental works 33,34 . In addition, Refs.…”
Section: Introductionmentioning
confidence: 98%
“…The very appealing property of a localized mode with a locked disorder-insensitive frequency has generated a lot of interest in reproducing the behavior of the SSH model using acoustic wave systems. Most of the approaches to date are based on coupled resonator systems [8][9][10][11][12][13]. There, to mimic the SSH model, the resonating acoustic cavities play the role of the atoms and the hoppings are realized by connecting tubes.…”
Section: Introductionmentioning
confidence: 99%