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引用次数: 0

摘要

本文报道了一种新型声子晶体(PnC)在$1\ \mu \mathrm{m}$氮化铝(AlN)薄膜上引起的局部机械共振。方形晶格中具有对角梁桥盘的非对称PnC在由连接梁的弯曲模态定义的PnC带隙内产生隔离模态。在这里,我们研究了PnC色散关系作为关键设计参数的函数的性质,定义了激发局域模式的谐振腔。具有156 MHz局域模式的PnC谐振器的特征是中心杆旋转角度($\theta$),驱动层数($\mathrm{N}_{act}$)和横向周期(P)的函数。这种具有设计的平坦色散关系的机电模式分析是实现近零密度(DNZ)超材料和芯片上弹性弹性波操作的重要第一步。
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Localized Modes in Asymmetric Phononic Crystals
This paper reports on a localized mechanical resonance induced by a novel phononic crystal (PnC) design demonstrated in a $1\ \mu \mathrm{m}$ aluminum nitride (AlN) thin film. An asymmetric PnC with diagonal beam bridging discs in a square lattice generates an isolated mode inside the PnC bandgap defined by the flexural mode of the connecting beam. Here we investigate the properties of the PnC dispersion relations as a function of key design parameters, defining resonance cavities to excite the localized mode. PnC resonators with localized mode at 156 MHz are characterized as a function of central bar rotation angle ($\theta$), number of actuation layers ($\mathrm{N}_{act}$) and lateral periods (P). This analysis of electromechanical modes with designed flat dispersion relation is an important first step toward Density-Near-Zero (DNZ) metamaterials and resilient elastic wave manipulation on chip.
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