2013
DOI: 10.1063/1.4801890
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Acoustic wave localization in one-dimensional Fibonacci phononic structures with mirror symmetry

Abstract: This paper reports on numerical and experimental results of acoustic transmission spectra of bead chains with symmetric and asymmetric Fibonacci-like structures. As a matter of comparison, perfect periodic acoustic waveguide structures are also examined. This study shows that Fibonacci structures with mirror symmetry can exhibit localized modes with higher amplitude, due to resonant transmission induced by the presence of dimers inside the 1D structure. A good agreement is observed between the theoretical pred… Show more

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Cited by 26 publications
(28 citation statements)
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“…Herein, the use of compressive integral projection to decompose the high-frequency spatial component of the initial target image can provide a solution restoring the desired target image (Fig. S7B-ii Therefore, the structures are a promising tool for exploring the physics of wave transport and controlling the properties of wave patterns, which are relevant to several areas of acoustic metasurfaces [34], wave localisation [39,40], tunable multiband responses of quasilattice metasurfaces [41], and chiral structures [35]. Considering an exposure area of several square milimetres and a lateral feature size similar to that of the single-aperture imaging-based PµSL configuration [11,12], the areal ratio (~10 2 ) of printing scales demonstrates that this imaging approach can be scaled without reducing optical resolution.…”
Section: Resultsmentioning
confidence: 99%
“…Herein, the use of compressive integral projection to decompose the high-frequency spatial component of the initial target image can provide a solution restoring the desired target image (Fig. S7B-ii Therefore, the structures are a promising tool for exploring the physics of wave transport and controlling the properties of wave patterns, which are relevant to several areas of acoustic metasurfaces [34], wave localisation [39,40], tunable multiband responses of quasilattice metasurfaces [41], and chiral structures [35]. Considering an exposure area of several square milimetres and a lateral feature size similar to that of the single-aperture imaging-based PµSL configuration [11,12], the areal ratio (~10 2 ) of printing scales demonstrates that this imaging approach can be scaled without reducing optical resolution.…”
Section: Resultsmentioning
confidence: 99%
“…A typical example are also generic solid state nanostructures [18], where unavoidable impurities and defects (usually modeled as P-symmetric) separate the host crystal into finite K-symmetric parts. LS may further be present by design in artificial devices like, e. g., multilay-ered photonic setups [19,20], acoustic waveguides [21,22], or magnonic systems [23], due to restrictions of finiteness or functionality. In fact, even global spatial symmetry is generally rendered local as soon as a system's immediate environment is included in the description.…”
Section: Introductionmentioning
confidence: 99%
“…These symmetry-induced spatial invariants were shown to enable a mapping of wave amplitudes of scattering states [17] or basis functions [18] between symmetryrelated points within any local symmetry (LS) domain. They have also been used to classify perfect transmission resonances [19] and as an order parameter for spontaneous symmetry breaking in parity-time symmetric scattering [20] and apply to a large variety of systems described by a spatial Helmholtz equation as e. g. in classical optics [21], quantum scattering [19], or even acoustic wave propagation [22][23][24] where it was readily corroborated by experiments [25]. As the invariant two-point currents are calculated from the stationary states, the LS formalism was so far -by construction-restricted to time-independent setups, thus making its generalization to time-dependent systems an intriguing yet challenging task.…”
mentioning
confidence: 99%