Spatial Decomposition of a Broadband Pulse Caused by Strong Frequency Dispersion of Sound in Acoustic Metamaterial Superlattice
An acoustic metamaterial superlattice is used for the spatial and spectral deconvolution of a broadband acoustic pulse into narrowband signals with different central frequencies. The operating frequency range is located on the second transmission band of the superlattice. The decomposition of the br...
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doaj-f12c80528bf24bf385249cb80a23ecd82020-12-31T00:02:41ZengMDPI AGMaterials1996-19442021-12-011412512510.3390/ma14010125Spatial Decomposition of a Broadband Pulse Caused by Strong Frequency Dispersion of Sound in Acoustic Metamaterial SuperlatticeYuqi Jin0Yurii Zubov1Teng Yang2Tae-Youl Choi3Arkadii Krokhin4Arup Neogi5Department of Physics, University of North Texas, P.O. Box 311427, Denton, TX 76203, USADepartment of Physics, University of North Texas, P.O. Box 311427, Denton, TX 76203, USADepartment of Physics, University of North Texas, P.O. Box 311427, Denton, TX 76203, USADepartment of Mechanical Engineering, University of North Texas, 3940 North Elm Suite, Denton, TX 76207, USADepartment of Physics, University of North Texas, P.O. Box 311427, Denton, TX 76203, USADepartment of Physics, University of North Texas, P.O. Box 311427, Denton, TX 76203, USAAn acoustic metamaterial superlattice is used for the spatial and spectral deconvolution of a broadband acoustic pulse into narrowband signals with different central frequencies. The operating frequency range is located on the second transmission band of the superlattice. The decomposition of the broadband pulse was achieved by the frequency-dependent refraction angle in the superlattice. The refracted angle within the acoustic superlattice was larger at higher operating frequency and verified by numerical calculated and experimental mapped sound fields between the layers. The spatial dispersion and the spectral decomposition of a broadband pulse were studied using lateral position-dependent frequency spectra experimentally with and without the superlattice structure along the direction of the propagating acoustic wave. In the absence of the superlattice, the acoustic propagation was influenced by the usual divergence of the beam, and the frequency spectrum was unaffected. The decomposition of the broadband wave in the superlattice’s presence was measured by two-dimensional spatial mapping of the acoustic spectra along the superlattice’s in-plane direction to characterize the propagation of the beam through the crystal. About 80% of the frequency range of the second transmission band showed exceptional performance on decomposition.https://www.mdpi.com/1996-1944/14/1/125acoustic metamaterialultrasound pulsepulse decompositionacoustic superlattice |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Yuqi Jin Yurii Zubov Teng Yang Tae-Youl Choi Arkadii Krokhin Arup Neogi |
spellingShingle |
Yuqi Jin Yurii Zubov Teng Yang Tae-Youl Choi Arkadii Krokhin Arup Neogi Spatial Decomposition of a Broadband Pulse Caused by Strong Frequency Dispersion of Sound in Acoustic Metamaterial Superlattice Materials acoustic metamaterial ultrasound pulse pulse decomposition acoustic superlattice |
author_facet |
Yuqi Jin Yurii Zubov Teng Yang Tae-Youl Choi Arkadii Krokhin Arup Neogi |
author_sort |
Yuqi Jin |
title |
Spatial Decomposition of a Broadband Pulse Caused by Strong Frequency Dispersion of Sound in Acoustic Metamaterial Superlattice |
title_short |
Spatial Decomposition of a Broadband Pulse Caused by Strong Frequency Dispersion of Sound in Acoustic Metamaterial Superlattice |
title_full |
Spatial Decomposition of a Broadband Pulse Caused by Strong Frequency Dispersion of Sound in Acoustic Metamaterial Superlattice |
title_fullStr |
Spatial Decomposition of a Broadband Pulse Caused by Strong Frequency Dispersion of Sound in Acoustic Metamaterial Superlattice |
title_full_unstemmed |
Spatial Decomposition of a Broadband Pulse Caused by Strong Frequency Dispersion of Sound in Acoustic Metamaterial Superlattice |
title_sort |
spatial decomposition of a broadband pulse caused by strong frequency dispersion of sound in acoustic metamaterial superlattice |
publisher |
MDPI AG |
series |
Materials |
issn |
1996-1944 |
publishDate |
2021-12-01 |
description |
An acoustic metamaterial superlattice is used for the spatial and spectral deconvolution of a broadband acoustic pulse into narrowband signals with different central frequencies. The operating frequency range is located on the second transmission band of the superlattice. The decomposition of the broadband pulse was achieved by the frequency-dependent refraction angle in the superlattice. The refracted angle within the acoustic superlattice was larger at higher operating frequency and verified by numerical calculated and experimental mapped sound fields between the layers. The spatial dispersion and the spectral decomposition of a broadband pulse were studied using lateral position-dependent frequency spectra experimentally with and without the superlattice structure along the direction of the propagating acoustic wave. In the absence of the superlattice, the acoustic propagation was influenced by the usual divergence of the beam, and the frequency spectrum was unaffected. The decomposition of the broadband wave in the superlattice’s presence was measured by two-dimensional spatial mapping of the acoustic spectra along the superlattice’s in-plane direction to characterize the propagation of the beam through the crystal. About 80% of the frequency range of the second transmission band showed exceptional performance on decomposition. |
topic |
acoustic metamaterial ultrasound pulse pulse decomposition acoustic superlattice |
url |
https://www.mdpi.com/1996-1944/14/1/125 |
work_keys_str_mv |
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