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Effects of dipolar scatterer orientation beside a plasmonic nanosphere in excitation rate enhancement

机译:等离子纳米球旁的偶极散射体取向对激发速率增强的影响

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Light scattering by plasmonic nanoparticles for enhancing the optical interactions, such as absorption, fluorescence, and Raman scattering have been under fervent study from different aspects. However, the scattering mechanism of a dipolar scatterer (DS) like a dye molecule or a quantum dot in the excitation regime is almost neglected in previous work for being very small. Stressing that scattering though small cannot be neglected in a system involving coupled components, we consider this mechanism in excitation rate evaluation of a generally oriented DS beside a plasmonic nanosphere (PN). In particular, we compare the two cases of radially and tangentially oriented DSs with respect to the surface of the PN. In this regard, the DS is assumed to express the polarizability only along its main axis, thus the induced dipole moment orientation is constant for a given DS with fix orientation (i.e. not rotating in the host medium). Furthermore, the polarizability of the DS is assumed to have a Lorentzian shape versus frequency.
机译:由等离子体纳米颗粒用于增强光学相互作用的光散射,例如吸收,荧光和拉曼散射一直处于不同方面的热烈研究。然而,在先前的工作中,偶极散射体(DS)如染料分子或激发系统中的量子点在非常小的工作中几乎忽略了散射机制。在涉及偶联组分的系统中,强调散射虽然小不能忽略散射,但我们认为这种机制在激励率评价中的激发速率评价在等离子体纳米末(PN)旁边的大致取向的DS。特别地,我们比较了径向和切向定向的DSS相对于PN的表面的两个情况。在这方面,假设DS仅沿其主轴表达极化性,因此诱导的偶极力矩取向对于具有固定方向的给定DS的常数(即,在主介质中不旋转)。此外,假设DS的极化性具有Lorentzian形状与频率。

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