Acoustic metamaterials and phononic crystals: Towards the total control of the wave propagation

A. Khelif
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引用次数: 3

Abstract

Classical waves, including elastic waves (acoustic waves) and electromagnetic waves (optical waves and microwaves), are described by conventional wave-propagation functions. Elastic waves were the first waveforms to be understood in condensed matter and have a wide range of applications from industry to defense, from healthcare to entertainment. In 1987, the photonic crystal was proposed to describe the propagation of optical waves in refraction index-modulated periodic structures analogous to the propagation of electrons in real crystals. This situation recalls the classical work by Brillouin. Brillouin considered elastic waves in periodic strings, electromagnetic waves in electrical circuits, and electrons in crystals as a system, resulting in some important common concepts, such as the Brillouin zone, band gap, etc., which are generally shared by the various forms of waves: electrons as scalar waves, optical waves as vector waves, and elastic waves as tensor waves. Following on from photonic crystals, the concept of phononic crystals was conceived with elastic waves propagating in periodic structures modulated with periodic elastic moduli and mass densities. These artificially structured materials possess a number of important properties, such as band gaps, band edge states7, and the ability to slow the velocity of sound (slow wave effect). Furthermore, by creating artificially designed structures on a deep subwavelength scale, artificial acoustic `atoms' can be purposely engineered into acoustic metamaterials to dramatically change the excitation and propagation of acoustic waves, and thus give rise to subdiffraction-limited resolution and its related myriad novel effects, such as negative, negative elastic modulus, and negative mass density. Finally, Acoustic metamaterials and phononicc crystal are a newly emerging field, which have inherently abnormal and interesting physical effects that are important to basic research, and offer potential for applications in everyday life that might revolutionize acoustic materials.
声学超材料与声子晶体:迈向波传播的完全控制
经典波,包括弹性波(声波)和电磁波(光波和微波),是用传统的波传播函数来描述的。弹性波是第一个在凝聚态物质中被理解的波形,从工业到国防,从医疗保健到娱乐都有广泛的应用。1987年,人们提出了光子晶体来描述光波在折射率调制周期结构中的传播,类似于电子在真实晶体中的传播。这种情况让人想起布里渊的经典作品。布里渊把周期弦中的弹性波、电路中的电磁波和晶体中的电子看作一个系统,从而产生了一些重要的共同概念,如布里渊带、带隙等,这些概念一般为各种形式的波所共有:电子为标量波,光波为矢量波,弹性波为张量波。继光子晶体之后,声子晶体的概念是由弹性波在周期性结构中传播,由周期性弹性模量和质量密度调制。这些人工结构的材料具有许多重要的特性,如带隙、带边状态和减慢声速的能力(慢波效应)。此外,通过在深亚波长尺度上创建人工设计的结构,人工声学“原子”可以被有意地设计成声学超材料,以显着改变声波的激发和传播,从而产生亚衍射极限分辨率及其相关的无数新效应,如负、负弹性模量和负质量密度。最后,声学超材料和声子晶体是一个新兴的领域,它们具有固有的异常和有趣的物理效应,对基础研究很重要,并且在日常生活中提供了潜在的应用,可能会彻底改变声学材料。
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