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60 Modeling Additive Color Effect in Natural Photonic Polycrystals Using the Layer Homogenization Method: The Case of the Diamond Weevil

机译:60使用层均质化方法在天然光子多晶中建模添加性颜色效果:钻石象鼻虫的情况

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The original method we propose allows to compute the spectral reflectance of photonic crystals whose unit cell is composed of form-birefringence anisotropic elements such as cylinders or parallelepipeds. This method relies on the layer homogenization of the photonic structure. It is especially useful for the calculation of reflectance according to different crystal orientations. The coloration due to an additive color effect in the photonic polycrystal found on the diamond weevil, Entimus imperialis, was investigated. Simulating the reflectance of photonic polycrystals often turns out to be necessary in the study of such structures as well as in the design and production of bioinspired devices (Vigneron and Lousse, Proc SPIE 6128:61281G, 2006; Deparis and Vigneron, Mater Sci Eng B-Adv 169(1-3): 12-15, 2010). In this context, the computation of the reflectance of photonic crystals (PCs) displaying form-birefringence anisotropic elements in the unit cell (e.g., cylinders, parallelepipeds...) turns out to be cumbersome, particularly when the reflectance is calculated for different crystal orientations as in the case of polycrystals. The method proposed here solves this problem in the particular case of a PC with a periodicity that is such that there is only specular reflection and no higher-order diffraction (Mouchet et al. Opt Express 21(11): 13228-13240, 2013). In this method, the structure with a particular crystal orientation is sliced into layers and the periodic dielectric function ε (→) is homogenized within each layer (Fig. 60.1a). Using this Layer Homogenization(LH) method, the reflectance of one single domain of the polycrystal can be computed in an arbitrary orientation thanks to a standard thin film solver. The reflectance due to the additive color effect created by the disorder in the crystal domain orientation of the polycrystal is modeled by averaging reflectance spectra computed for several incidence angles and crystal domain orientations. Our method
机译:我们提出的原始方法允许计算光子晶体的光谱反射率,其单位电池由诸如汽缸或平行六面体的形式 - 双折射各向异性元件组成。该方法依赖于光子结构的层均匀化。根据不同的晶体取向,它特别适用于计算反射率。研究了在钻石象鼻虫,entimusimialis上发现的光子多晶中的添加性颜色效果引起的着色。模拟光子多晶的反射率经常在研究这些结构以及生物悬浮装置的设计和生产方面是必要的(Vigneron和Lousse,Proc Spie 6128:61281G,2006; Deparis和Vigneron,Mater Sci Eng B. - 签变169(1-3):12-15,2010)。在这种情况下,在单元电池(例如,圆柱体,平行六面积...)中显示光子晶体(PCS)的反射率在单元电池(例如,圆柱体,平行六面积...)中的反射率变为麻烦,特别是当对不同晶体计算反射率时在多晶的情况下取向。本文所提出的方法在具有周期性的PC的特定情况下解决了该问题,使得只有镜面反射并且没有高阶衍射(Mouchet等,Opt Express 21(11):13228-13240,2013) 。在该方法中,将具有特定晶体取向的结构切成薄层,并且周期性介电功能ε(→)在每个层内均化(图60.1a)。使用该层均质化(LH)方法,由于标准薄膜求解器,可以以任意取向计算多个晶体的一个单个结构域的反射率。由于由多晶体的晶体畴取向产生的晶体畴取向而产生的反射率是通过为几个入射角和晶体畴方向计算的反射光谱来建模。我们的方法

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