Analysis of Band Structures of Nanosized Phononic Crystals by Nonlocal Elastic Theory

Author(s):  
Yue-Sheng Wang ◽  
A-Li Chen

Based on the nonlocal elastic continuum theory, the band structures of the nano-sized layered phononic crystals are analyzed by computing the localization factors and dispersion curves. Detailed calculations are performed for a nanosized HfO2–ZrO2 periodic layer stack. The size-effect on the band structures is examined. It is found that the nonlocal elastic continuum solution deviates from the classical elastic continuum theory and finally approaches the first-principle result as the thickness of each individual layer decreases. Due to the size-effect, there exists a cut-off frequency beyond which the waves cannot propagate through the system.

2012 ◽  
Vol 376 (33) ◽  
pp. 2256-2263 ◽  
Author(s):  
Zhenlong Xu ◽  
Fugen Wu ◽  
Zhongning Guo

Author(s):  
Zi-Gui Huang ◽  
Yunn-Lin Hwang ◽  
Pei-Yu Wang ◽  
Yen-Chieh Mao

The excellent applications and researches of so-called photonic crystals raise the exciting researches of phononic crystals. By the analogy between photon and phonon, repetitive composite structures that are made up of different elastic materials can also prevent elastic waves of some certain frequencies from passing by, i.e., the frequency band gap features also exist in acoustic waves. In this paper, we present the results of the tunable band gaps of acoustic waves in two-dimensional phononic crystals with reticular band structures using the finite element method. Band gaps variations of the bulk modes due to different thickness and angles of reticular band structures are calculated and discussed. The results show that the total elastic band gaps for mixed polarization modes can be enlarged or reduced by adjusting the orientation of the reticular band structures. The phenomena of band gaps of elastic or acoustic waves can potentially be utilized for vibration-free, high-precision mechanical systems, and sound insulation.


Meccanica ◽  
2017 ◽  
Vol 53 (4-5) ◽  
pp. 923-935 ◽  
Author(s):  
Ying Wu ◽  
Kaiping Yu ◽  
Linyun Yang ◽  
Rui Zhao

Nanomaterials ◽  
2020 ◽  
Vol 10 (11) ◽  
pp. 2205
Author(s):  
Ilyasse Quotane ◽  
El Houssaine El Boudouti ◽  
Bahram Djafari-Rouhani

In this paper, we provide a theoretical and numerical study of the acoustic properties of infinite and semi-infinite superlattices made out of graphene-semiconductor bilayers. In addition to the band structure, we emphasize the existence and behavior of localized and resonant acoustic modes associated with the free surface of such structures. These modes are polarized in the sagittal plane, defined by the incident wavevector and the normal to the layers. The surface modes are obtained from the peaks of the density of states, either inside the bulk bands or inside the minigaps of the superlattice. In these structures, the two directions of vibrations (longitudinal and transverse) are coupled giving rise to two bulk bands associated with the two polarizations of the waves. The creation of the free surface of the superlattice induces true surface localized modes inside the terahertz acoustic forbidden gaps, but also pseudo-surface modes which appear as well-defined resonances inside the allowed bands of the superlattice. Despite the low thickness of the graphene layer, and though graphene is a gapless material, when it is inserted periodically in a semiconductor, it allows the opening of wide gaps for all values of the wave vector k// (parallel to the interfaces). Numerical illustrations of the band structures and surface modes are given for graphene-Si superlattices, and the surface layer can be either Si or graphene. These surface acoustic modes can be used to realize liquid or bio-sensors graphene-based phononic crystal operating in the THz frequency domain.


2014 ◽  
Vol 23 ◽  
pp. 63-71 ◽  
Author(s):  
Fang-Guang Kuang ◽  
Xiao-Yu Kuang ◽  
Shu-Ying Kang ◽  
Ming-Min Zhong ◽  
Ai-Jie Mao

Crystals ◽  
2016 ◽  
Vol 6 (1) ◽  
pp. 11 ◽  
Author(s):  
Lin Han ◽  
Yan Zhang ◽  
Xiao-mei Li ◽  
Lin-hua Jiang ◽  
Da Chen

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