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Floquet-mode analysis of pillar-type photonic crystal waveguide using spectral-domain approach

机译:光谱域法分析柱型光子晶体波导的浮球模式

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Photonic crystal is a periodic structure consisting of highly contrast dielectrics, in which the electromagnetic wave cannot transmit in a specific wavelength range. It is therefore known that, if localized defects are introduced in the photonic crystal, the electromagnetic fields are strongly confined around the defects. For example, point defects in the photonic crystal work as resonance cavities and line defects work as waveguides. This paper presents a Floquet-mode analysis of the photonic crystal waveguide (PCW) using the spectral-domain approach. For the straight waveguides, the structure maintains the periodicity in the propagation direction, and the Floquet theorem asserts that the electromagnetic fields in the structure can be expressed by superposition of the Floquet-modes [1]. The Floquet-modes of the PCW are obtained by the eigenvalue analysis of the transfer matrix for one periodicity cell in the propagation direction. The periodicity cell that makes up the PCW has imperfect periodicity in the direction perpendicular to wave propagation. Therefore the fields in the structure have continuous spectra. The present analysis uses the pseudo-periodic Fourier transform (PPFT) [2] to consider the discretization scheme in the wavenumber space. The PPFT and its inverse are formally given by f(x; ξ) = Σm = −∞ f (x − md)eimdξ (1) f(x) = 1/kd ∫kd/2−kd/2 f(x; ξ)d ξ (2) where d is a positive value usually chosen to be equal with the structural period, ξ is a transform parameter, and kd = 2π/d is the inverse lattice constant.
机译:光子晶体是由高对比度电介质组成的周期性结构,其中电磁波无法在特定的波长范围内传输。因此,已知如果在光子晶体中引入局部缺陷,则电磁场被强烈地限制在缺陷周围。例如,光子晶体中的点缺陷充当谐振腔,而线缺陷充当波导。本文介绍了使用光谱域方法对光子晶体波导(PCW)进行浮球模式分析。对于直波导,该结构在传播方向上保持周期性,Floquet定理断言该结构中的电磁场可以通过Floquet模式的叠加来表示[1]。通过在传播方向上对一个周期单元的传输矩阵进行特征值分析,可以获得PCW的Floquet模式。组成PCW的周期性单元在垂直于波传播的方向上具有不完善的周期性。因此,结构中的场具有连续的光谱。本分析使用伪周期傅里叶变换(PPFT)[2]考虑波数空间中的离散化方案。 PPFT及其倒数的形式为f(x;ξ)=Σ m =-∞f(x-md)e imdξ(1)f(x )= 1 / kd∫ kd / 2 -kd / 2 f(x;ξ)dξ(2)其中d是通常选择为与结构周期相等的正值,ξ是a变换参数,并且kd =2π/ d是逆晶格常数。

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