含金属夹杂的一维光子晶体的空间色散效应

F. Perez Rodriguez, F. Diaz Monge, N. M. Makarov, R. Marquez Islas, B. F. Desirena
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引用次数: 1

摘要

从理论上研究了金属-介质和金属-半导体一维光子晶体的光谱特性,分别考虑了金属和半导体中的空间色散。在由金属板和介电板交替组成的一维等离子体中,为了确定金属板的非局部本构方程,我们将玻尔兹曼动力学方程的经典形式应用于导电电子分布函数。然后,我们计算了一维PC中体模的色散关系,并将其与隐式局部的德鲁德-洛伦兹模型中得到的色散关系进行了比较。以金属半导体一维PC为例,研究了另一种非局域效应。在这种情况下,金属元件的频率相关介电函数由局部德鲁德-洛伦兹模型描述,而对于半导体,我们使用Hopfield-Thomas介电函数,它描述了其在激子共振附近的非局部行为。比较了金属半导体光子晶体中s偏振模式的极化子色散曲线与金属介电光子晶体的色散曲线。由于光与激子的耦合,激子在薄半导体板内进行尺寸量子化,出现了许多光子小带。研究了金属填充量不同时,谐振一维PC的光子色散曲线的变化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spatial-Dispersion Effects in One-Dimensional Photonic Crystals with Metallic Inclusions
The spectral properties of metal-dielectric and metal-semiconductor 1D photonic crystals (PCs) are theoretically investigated, considering spatial dispersion in the metal and in the semiconductor, respectively. In the case of 1D PCs, composed of alternating metallic and dielectric slabs, we apply the classical formalism of the Boltzmann's kinetic equation for the distribution function of the conduction electrons in order to determine the nonlocal constitutive equation for the metallic slabs. Afterwards, we calculate the dispersion relation for the bulk modes in the 1D PC and compare it with that obtained within the Drude-Lorentz model, which is implicitly local. Another kind of nonlocal effects are studied by considering a metal-semiconductor 1D PC. In this case, the frequency-dependent dielectric function of the metallic component is described by the local Drude-Lorentz model, whereas for the semiconductor we use a Hopfield-Thomas dielectric function, which describes its nonlocal behavior near exciton resonance. The polariton dispersion curves for s-polarized modes in the metal- semiconductor photonic crystal are compared with those for a metal-dielectric PC. Because of the coupling of light with excitons, which undergo size quantization inside the thin semiconductor slabs, many photonic small bands appear. We study the changes in the photonic dispersion curves for the resonant 1D PC as the filling fraction of the metal is varied.
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