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二维介质柱型阿基米德复式晶格光子晶体禁带特性

Bandgap characteristics of two-dimensional Archimedean compound lattice photonic cystals with dielectric rods

中文摘要英文摘要

采用平面波展开法(PWM)模拟由介质圆柱和方柱构造的二维Archimedes (4,82)复式晶格光子晶体的能带结构,分别讨论折射率、介质柱形状、填充比和旋转对称性对光子晶体完全禁带的影响。研究发现,在折射率为2.60到5.4之间,介质圆柱和介质方柱构造的的二维Archimedes (4,82)复式晶格光子晶体都出现了完全光子禁带。随折射率的增大,介质圆柱构造的的二维Archimedes (4,82)复式晶格在折射率n=2.80时出现一个禁带峰值;介质方柱型在折射率n=2.80和n=4.40出现两处禁带峰值,且旋转介质方柱能够明显增大禁带宽度。分析结果表明,通过改变折射率和介质填充比等结构参数可以调制光子晶体完全禁带中心频率位置、带宽及禁带数目。

he bandgaps of the two-dimensional Archimedes (4,82) lattice consisting of different dielectric circular and square rods are calculated with the plane wave expansion method. The bandgaps of the lattice with dielectric rods are also investigated as the refractive index, dielectric rods shape, filling fraction and rotational symmetry changing. it was found that complete photonic bandgaps can be achieved in the (4,82) structure when the refractive index is between 2.60 and 5.40. For the Archimedes (4,82) lattice of circular dielectric rod, the width of complete bandgap reaches the maximum at the dielectric refractive index of rod is equal to 2.80. Also, the complete bandgap of square dielectric rod reaches the maximum when the dielectric refractive index equals 2.80 or 4.40. in addition, the rotation angle of square dielectric rods can significantly increase the width of complete bandgap. The results demonstrate that the quantity, width and frequency position of bandgaps can be modulated by changing the refractive index, the filling fraction and other structural parameters.

王伟军、杨毅彪

物理学晶体学光电子技术

光学光子晶体完全光子禁带rchimedes结构平面波展开法

opticsphotonic crystalscomplete bandgapArchimedean latticeplane wave expansion method

王伟军,杨毅彪.二维介质柱型阿基米德复式晶格光子晶体禁带特性[EB/OL].(2011-10-11)[2025-08-21].http://www.paper.edu.cn/releasepaper/content/201110-66.点此复制

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