2011
DOI: 10.1016/j.ssc.2010.12.008
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Acoustic tunneling through artificial structures: From phononic crystals to acoustic metamaterials

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Cited by 11 publications
(6 citation statements)
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“…A careful design of the micro-level architecture enables metamaterials to provide exceptional macro-behavior, properties, and functionalities that surpass those of standard materials. [6] For more than two decades, metamaterials that manipulate optical, [7,8] acoustic, [9] and thermal [10] fields as well as stress waves, [11][12][13] and that have highly unusual properties, such as a "negative mass" [14][15][16] or ultra-high stiffness to weight ratio [17] have attracted a great deal of attention. Multistable metamaterials, consisting of an array of bistable units, are a promising class of mechanical metamaterials.…”
Section: Doi: 101002/adma202301483mentioning
confidence: 99%
“…A careful design of the micro-level architecture enables metamaterials to provide exceptional macro-behavior, properties, and functionalities that surpass those of standard materials. [6] For more than two decades, metamaterials that manipulate optical, [7,8] acoustic, [9] and thermal [10] fields as well as stress waves, [11][12][13] and that have highly unusual properties, such as a "negative mass" [14][15][16] or ultra-high stiffness to weight ratio [17] have attracted a great deal of attention. Multistable metamaterials, consisting of an array of bistable units, are a promising class of mechanical metamaterials.…”
Section: Doi: 101002/adma202301483mentioning
confidence: 99%
“…While made from standard materials, the geometry of their building blocks can give rise to unique behaviors 5 . For example, metamaterials have been designed to have "negative mass" [6][7][8] , to manipulate light 9,10 and stress waves [11][12][13] , or to provide ultra-high stiffness to weight ratio 14 . Multistable meta-materials feature a multitude of possible equilibrium configurations for a prescribed load.…”
Section: Introductionmentioning
confidence: 99%
“…Figures 3(c) and (d) demonstrate the filed distributions while the source vibrates at the frequencies ω s a/2πc t = 0.207 and ω s a/2πc t = 0.276, respectively. Because of the tunnelling [34], more energy will leak out from the waveguide at high frequencies, where the absolute value of ρ y eff gets smaller.…”
mentioning
confidence: 99%