Abstract:We demonstrate both theoretically and experimentally the physical mechanism that underlies extraordinary acoustic transmission and collimation of sound through a one-dimensional decorated plate. A microscopic theory considers the total field as the sum of the scattered waves by every periodically aligned groove on the plate, which divides the total field into far-field radiative cylindrical waves and acoustic surface evanescent waves (ASEWs). Different from the well-known acoustic surface waves like Rayleigh w… Show more
“…Note that the dipole-like radiation phenomenon occurs when the wavelength (l ¼ 40 mm) is much larger than the period of the HRs (d ¼ 8 mm), which can be utilized to realize device miniaturization. As no sidelobes occur in the pattern, the pattern is not due to the excitation of the acoustic surface wave emerging only in the vicinity of the resonant transmission peak 20 . Actually, the dipole-like radiation pattern can occur in a very wide bandwidth, which is illustrated below.…”
Section: Resultsmentioning
confidence: 99%
“…It may seem that our system is similar to that of a single slit surrounded by finite, periodically perforated grooves; however, the experimental phenomenon and the mechanism of our system are quite different. The directional beam experimental report by Zhou et al 20 showed very strong fingerprints of the running surface wave scattered by the grooves [20][21][22] , and the directional beam occurred in a very narrow bandwidth. We verify that the dipole-like pattern radiation phenomenon in our samples arises from the effective boundary impedance adjustment.…”
Radiation pattern control has generated much interest recently due to its potential applications. Here we report the observation of high-efficiency dipole-like radiation of sound with broad bandwidth through a decorated plate with periodical two-dimensional Helmholtz resonators on both sides and a single slit at the centre. The decorated plate was optimally designed to adjust the effective impedance of the boundary, and the underlying mechanism of radiation pattern control is attributed to wave vector tailoring. The high radiation efficiency is due to the Fabry-Perot resonances associated with waveguide modes in the centre slit. The method to obtain a collimated beam without any sidelobes is also provided. Our findings should have an impact on acoustic applications.
“…Note that the dipole-like radiation phenomenon occurs when the wavelength (l ¼ 40 mm) is much larger than the period of the HRs (d ¼ 8 mm), which can be utilized to realize device miniaturization. As no sidelobes occur in the pattern, the pattern is not due to the excitation of the acoustic surface wave emerging only in the vicinity of the resonant transmission peak 20 . Actually, the dipole-like radiation pattern can occur in a very wide bandwidth, which is illustrated below.…”
Section: Resultsmentioning
confidence: 99%
“…It may seem that our system is similar to that of a single slit surrounded by finite, periodically perforated grooves; however, the experimental phenomenon and the mechanism of our system are quite different. The directional beam experimental report by Zhou et al 20 showed very strong fingerprints of the running surface wave scattered by the grooves [20][21][22] , and the directional beam occurred in a very narrow bandwidth. We verify that the dipole-like pattern radiation phenomenon in our samples arises from the effective boundary impedance adjustment.…”
Radiation pattern control has generated much interest recently due to its potential applications. Here we report the observation of high-efficiency dipole-like radiation of sound with broad bandwidth through a decorated plate with periodical two-dimensional Helmholtz resonators on both sides and a single slit at the centre. The decorated plate was optimally designed to adjust the effective impedance of the boundary, and the underlying mechanism of radiation pattern control is attributed to wave vector tailoring. The high radiation efficiency is due to the Fabry-Perot resonances associated with waveguide modes in the centre slit. The method to obtain a collimated beam without any sidelobes is also provided. Our findings should have an impact on acoustic applications.
“…A motion picture showing the frequency dependence of the emitted beam propagating in free space is presented in the Supplemental Material Movie S3 [7]. This is not the first demonstration of funneling of acoustic energy with perforated structures, but the previous one [14,15] and the phenomenon was obtained resonantly, using acoustic surface waves. Here, on the contrary, it is a nonresonant phenomenon and consequently its bandwidth is not strongly limited.…”
“…Novel phenomena have been investigated, for example, enhanced light-matter interaction, ultrafast acoustoplasmonic control, and sensing by evanescent surface acoustic waves (SAWs). [1][2][3][4] Phononic nanostructures could lead to a variety of potential applications, ranging from acoustic metamaterials, self-collimation, sound isolation, and heat management to compact acoustic waveguides. [5][6][7][8][9] Similar to their photonic counterparts, the flexibility to tailor the acoustic properties of phononic crystals (PnCs) and PnC waveguides makes them particularly suitable for a wide range of applications from transducer technology to filtering, guiding, and demultiplexing of acoustic waves.…”
The study of surface modes in phononic crystal waveguides in the hypersonic regime is a burgeoning field with a large number of possible applications. By using the finite element method, the band structure and the corresponding transmission spectrum of surface acoustic waves in phononic crystal waveguides generated by line defects in a silicon pillar-substrate system were calculated and investigated. The bandgaps are caused by the hybridization effect of band branches induced by local resonances and propagating modes in the substrate. By changing the sizes of selected pillars in the phononic crystal waveguides, the corresponding bands shift and localized modes emerge due to the local resonance effect induced by the pillars. This effect offers further possibilities for tailoring the propagation and filtering of elastic waves. The presented results have implications for the engineering of phonon dynamics in phononic nanostructures.
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