Optical response of azopolymer (PAZO) layers doped with TiO2 nanoparticles

N. Berberova, P. Sharlandjiev, D. Nazarova, L. Nedelchev
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引用次数: 1

Abstract

In this paper we analyze the optical response of azopolymer (poly[1-[4-(3-carboxy-4-hydroxyphenylazo) benzenesulfonamido] -1,2-ethan-ediyl, sodium salt]), shortly denoted as PAZO. The photoinduced birefringence of this material has a potential for polarization holographic recording. We consider thin PAZO layers with embedded TiO2 spherical particles. This is a numeric simulation motivated by the search of photoinduced birefringence enhancement in azopolymer layers. The scattering of a single particle in the dye-polymer matrix is calculated using the exact vector Maxwell equations. The particles are treated as ensemble of non-aggregated spheres with normal distribution of sizes, characterized by the mean radius /4. Multiple scattering by individual particles is ignored. The refractive index of the PAZO matrix at 442 nm has a complex value (due to absorption) as we have determined it from experimental spectrophotometric data. The 442 nm wavelength is commonly used for recording polarization holographic gratings in azopolymer materials. Embedded TiO2 spheres with mean radius from 10 to 80 nm are considered. The angular dependences of all the scattering matrix elements, which describe the optical response of the composite layers, are estimated.
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掺杂TiO2纳米粒子的偶氮聚合物(PAZO)层的光学响应
本文分析了偶氮聚合物(聚[1-[4-(3-羧基-4-羟基苯基偶氮)苯磺胺]-1,2-乙二基,钠盐])的光学响应,简称为PAZO。该材料的光致双折射特性具有偏振全息记录的潜力。我们考虑嵌入TiO2球形颗粒的薄PAZO层。这是一个数值模拟的动机是寻找光诱导双折射增强在偶氮聚合物层。用精确的矢量麦克斯韦方程组计算了单个粒子在染料-聚合物基体中的散射。将颗粒视为大小为正态分布的非聚集球体的集合,其特征为平均半径/4。忽略单个粒子的多次散射。PAZO矩阵在442 nm处的折射率有一个复值(由于吸收),这是我们从实验分光光度法数据中确定的。442 nm波长通常用于偶氮聚合物材料的偏振全息光栅记录。考虑了平均半径为10 ~ 80 nm的包埋TiO2球。估计了描述复合材料层光学响应的所有散射矩阵元素的角依赖性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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