2011
DOI: 10.1063/1.3665205
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Large bandgaps of two-dimensional phononic crystals with cross-like holes

Abstract: In this paper we study the bandgap properties of two-dimensional phononic crystals with cross-like holes using the finite element method. The influence of the geometry parameters of the holes on the bandgaps is discussed. In contrast to a system of square holes, which does not exhibits bandgaps if the symmetry of the holes is the same as that of the lattice, systems of cross-like holes show large bandgaps at lower frequencies. The bandgaps are significantly dependent upon the geometry (including the size, shap… Show more

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Cited by 145 publications
(68 citation statements)
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“…The phononic band structure can be computed numerically using several methods such as multiple scattering theory [3,4], plane wave expansion [5][6][7], and finite element method [8][9][10]. However, it is also important to understand how the band structure forms and how it is affected by the geometry of the phononic crystal and properties of constituent materials.…”
Section: Introductionmentioning
confidence: 99%
“…The phononic band structure can be computed numerically using several methods such as multiple scattering theory [3,4], plane wave expansion [5][6][7], and finite element method [8][9][10]. However, it is also important to understand how the band structure forms and how it is affected by the geometry of the phononic crystal and properties of constituent materials.…”
Section: Introductionmentioning
confidence: 99%
“…A more practical and promising solution are single-phase metamaterials, which have attracted increasing interest in the community [29][30][31][32][33][34][35][36][37][38], and in which both types of BGs have been shown to be present [39][40][41][42][43]. However, to the best of our knowledge, the conditions and physical mechanism of the coupling of Bragg BG with local resonances in single-phase structures has not yet been analyzed.…”
Section: Introductionmentioning
confidence: 98%
“…The optimized structures can be modeled as mass-spring systems, i.e., the solid lumps act as masses and the bars as the springs. 59 It is seen from the modes O 1 , O 3 and O 5 that the lumps vibrate strongly and the bars vibrate slightly for the lower-edge modes. However, for the upper-edge modes O 2 , O 4 and O 6 , the situation is the reverse.…”
Section: Physical Mechanism Analysismentioning
confidence: 99%