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The properties of the extraordinary mode and surface plasmon modes in the three-dimensional magnetized plasma photonic crystals based on the magneto-optical Voigt effects

机译:基于磁光Voigt效应的三维磁化等离子体光子晶体中超常模和表面等离子体激元的性质

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In this paper, the properties of the extraordinary mode and surface plasmon modes in the threedimensional (3D) magnetized plasma photonic crystals (MPPCs) with face-centered-cubic lattices that are composed of the core tellurium (Te) spheres with surrounded by the homogeneous magnetized plasma shells inserted in the air, are theoretically investigated in detail by the plane wave expansion method, as the magneto-optical Voigt effects of magnetized plasma are considered (the incidence electromagnetic wave vector is perpendicular to the external magnetic field at any time). The optical switching or wavelength division multiplexer can be realized by the proposed 3D MPPCs. Our analyses demonstrate that the complete photonic band gaps (PBGs) and two flatbands regions for the extraordinary mode can be observed obviously. PBGs can be tuned by the radius of core Te sphere, the plasma density and the external magnetic field. The flatbands regions are determined by the existence of surface plasmon modes. Numerical simulations also show that if the thickness of magnetized plasma shell is larger than a threshold value, the band structures of the extraordinary mode will be similar to those obtained from the same structure containing the pure magnetized plasma spheres. In this case, the band structures also will not be affected by the inserted core spheres. It is also provided that the upper edges of two flatbands regions will not depend on the topology of lattice. However, the frequencies of lower edges of two flatbands regions will be convergent to the different constants for different lattices, as the thickness of magnetized plasma shell is close to zero.
机译:本文研究了具有以面心为中心的立方晶格的三维(3D)磁化等离子体光子晶体(MPPC)的超常模和表面等离振子模式的性质,这些晶格由核心碲(Te)球组成,并被均质包围考虑到磁化等离子体的磁光Voigt效应(入射电磁波矢量在任何时间都垂直于外部磁场),通过平面波扩展方法对插入空气中的磁化等离子体壳进行了理论上的详细研究。光开关或波分复用器可以通过提出的3D MPPC实现。我们的分析表明,可以明显观察到非常规模式的完整光子带隙(PBG)和两个平坦带区域。 PBG可以通过核心Te球的半径,等离子体密度和外部磁场来调整。平坦带区域由表面等离子体激元模的存在确定。数值模拟还表明,如果磁化等离子体壳的厚度大于阈值,则非常规模式的能带结构将类似于从包含纯磁化等离子体球的相同结构获得的能带结构。在这种情况下,带状结构也不会受到插入的芯球的影响。还规定,两个平坦带区域的上边缘将不取决于晶格的拓扑。然而,由于磁化等离子体壳的厚度接近于零,因此两个平坦带区域的下边缘的频率将收敛于不同晶格的不同常数。

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