2017
DOI: 10.1103/physrevlett.118.084302
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Harnessing Geometric Frustration to Form Band Gaps in Acoustic Channel Lattices

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Cited by 30 publications
(17 citation statements)
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“…This study represents the first step towards the investigation of large amplitude waves in beam lattices in 2D and 3D. While periodic lattices have recently attracted considerable interest because of their ability to tailor the propagation of linear elastic waves through directional transmissions and band gaps (frequency ranges of strong wave attenuation) [39][40][41][42][43], comparatively little is known about their nonlinear behaviors under high-amplitude impacts [20]. The results presented in this paper provide useful guidelines for future explorations of the propagation of nonlinear waves in lattice materials.…”
Section: Discussionmentioning
confidence: 99%
“…This study represents the first step towards the investigation of large amplitude waves in beam lattices in 2D and 3D. While periodic lattices have recently attracted considerable interest because of their ability to tailor the propagation of linear elastic waves through directional transmissions and band gaps (frequency ranges of strong wave attenuation) [39][40][41][42][43], comparatively little is known about their nonlinear behaviors under high-amplitude impacts [20]. The results presented in this paper provide useful guidelines for future explorations of the propagation of nonlinear waves in lattice materials.…”
Section: Discussionmentioning
confidence: 99%
“…To obtain the discrete equation (1), we assume that only the planar mode is propagating (i.e. R t /L = 1) in the acoustic waveguide, allowing us to write down the acoustic particle velocity at any end of the channel as a function of the pressure at both ends [36,37]. For example, as shown schematically in the right part of figure A1, we may write that…”
Section: Discussionmentioning
confidence: 99%
“…To obtain the governing equations and the dispersion properties for the acoustic network, we adopt the methodology initially proposed in 2D lattices of tubes [35] and further developed in 2D acoustic channels of lattice structures [36,37]. We assume that sound wave propagation between junctions is well described as monomode propagation (plane wave approximation) as long as the radius of the air channels is much smaller than the distance between the two junctions A and B, i.e.…”
Section: Exact Acoustic Analog Of Graphenementioning
confidence: 99%
“…Soon, people realized that similar phenomena are not restricted to quantum systems, and nontrivial topology can also bring exciting phenomena and results in classical wave systems. Recently, classical analogs of QSH and QVH insulators were predicted and verified both theoretically and experimentally in electromagnetic [3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18], acoustic [19][20][21][22][23][24][25][26][27][28][29][30][31][32][33], elastic [34][35][36][37][38][39][40][41][42][43], and even water surface wave systems [44]. Very recently, robust and high-capacity phononic communications were realized in the context of Lamb waves through topological edge states by multiplexing the pseudospin and valley indices [43].…”
Section: Introductionmentioning
confidence: 99%