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超低声学超宽带非线性声子晶体。

Ultra-low and ultra-broad-band nonlinear acoustic metamaterials.

机构信息

Laboratory of Science and Technology on Integrated Logistics Support, National University of Defense Technology, Changsha, Hunan, 410073, China.

Institut des NanoSciences de Paris (INSP-UMR CNRS 7588), Université Pierre et Marie Curie, (Box 840) 4, Place Jussieu, 75252, Paris Cedex 05, France.

出版信息

Nat Commun. 2017 Nov 3;8(1):1288. doi: 10.1038/s41467-017-00671-9.

DOI:10.1038/s41467-017-00671-9
PMID:29101396
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5670230/
Abstract

Linear acoustic metamaterials (LAMs) are widely used to manipulate sound; however, it is challenging to obtain bandgaps with a generalized width (ratio of the bandgap width to its start frequency) >1 through linear mechanisms. Here we adopt both theoretical and experimental approaches to describe the nonlinear chaotic mechanism in both one-dimensional (1D) and two-dimensional (2D) nonlinear acoustic metamaterials (NAMs). This mechanism enables NAMs to reduce wave transmissions by as much as 20-40 dB in an ultra-low and ultra-broad band that consists of bandgaps and chaotic bands. With subwavelength cells, the generalized width reaches 21 in a 1D NAM and it goes up to 39 in a 2D NAM, which overcomes the bandwidth limit for wave suppression in current LAMs. This work enables further progress in elucidating the dynamics of NAMs and opens new avenues in double-ultra acoustic manipulation.

摘要

线性声子晶体(LAMs)被广泛用于操控声波,然而,通过线性机制获得具有广义带宽(带隙宽度与起始频率之比)>1 的带隙是具有挑战性的。在这里,我们采用理论和实验的方法来描述一维(1D)和二维(2D)非线性声子晶体(NAMs)中的非线性混沌机制。该机制使得 NAMs 能够在超低频和超宽带范围内(由带隙和混沌带组成)将波的传输降低 20-40dB。通过亚波长单元,1D NAM 的广义带宽达到 21,2D NAM 的广义带宽达到 39,这克服了当前 LAMs 中对波抑制的带宽限制。这项工作促进了对 NAMs 动力学的进一步研究,并为双超声操控开辟了新途径。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/a1d4cd7a8799/41467_2017_671_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/ff78e1a518a8/41467_2017_671_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/a6f54c28c138/41467_2017_671_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/b57c34508ec7/41467_2017_671_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/c9280e55e93c/41467_2017_671_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/1305020e0d0b/41467_2017_671_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/a8d1e8b6f2f9/41467_2017_671_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/5ab4967a34fb/41467_2017_671_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/a1d4cd7a8799/41467_2017_671_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/ff78e1a518a8/41467_2017_671_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/a6f54c28c138/41467_2017_671_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/b57c34508ec7/41467_2017_671_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/c9280e55e93c/41467_2017_671_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/1305020e0d0b/41467_2017_671_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/a8d1e8b6f2f9/41467_2017_671_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/5ab4967a34fb/41467_2017_671_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d3d0/5670230/a1d4cd7a8799/41467_2017_671_Fig8_HTML.jpg

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