{"title":"Studying dipole moment modification in a single fluorescent dye beside metallic Nano-Particle based on the Green's function theory","authors":"F. T. Ladani, C. Guclu, S. Campione, F. Capolino","doi":"10.1109/USNC-URSI-NRSM.2013.6525098","DOIUrl":null,"url":null,"abstract":"Summary form only given. Enhancement of dipolar scattering can be achieved by locating the emitting dipole near a resonant nanosphere. In this study the dipole represents a fluorescent dye or an emitting quantum dot, and the nanosphere exhibits a plasmonic resonance at optical frequencies. It has been shown several times that a dipole excitation and emission can be greatly affected by the presence of a nanosphere at nanomener distance. This was considered for example in (J. Gersten, A. Nitzan, J. Chem. Phys. 73(7), 1980) in the case of Raman scattering, and in many other experimental works. In this paper, we investigate the emission of a fluorescent dye analytically, using the electric dyadic Green's function in a semiclassical electrodynamic model accounting for the nanosphere scattering, which is evaluated according to Mie theory. The dye is modeled as a dipole, illuminated by an incident wave and the one from the nearby nanosphere. We compare our results with previous ones, based on different approximations. More specifically, assuming the dipolar dye is located beside the NP, we analyze when the latter, in turn, modifies the dye dipole moment since the dye has a certain polarizability and hence responds to the local electric field. We report when this contribution is important for the determination of the dye emission rate and scattering. We use the Lorentzian oscillator model for calculating the polarizability of the dye and investigate excitation rate enhancements in various cases. As results show when the polarizability of the dye becomes comparable to that of the plasmonic nanosphere we have to consider the change in the dipole moment of the dye, as in our electrocynamic model.","PeriodicalId":123571,"journal":{"name":"2013 US National Committee of URSI National Radio Science Meeting (USNC-URSI NRSM)","volume":"91 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2013-06-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2013 US National Committee of URSI National Radio Science Meeting (USNC-URSI NRSM)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/USNC-URSI-NRSM.2013.6525098","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Summary form only given. Enhancement of dipolar scattering can be achieved by locating the emitting dipole near a resonant nanosphere. In this study the dipole represents a fluorescent dye or an emitting quantum dot, and the nanosphere exhibits a plasmonic resonance at optical frequencies. It has been shown several times that a dipole excitation and emission can be greatly affected by the presence of a nanosphere at nanomener distance. This was considered for example in (J. Gersten, A. Nitzan, J. Chem. Phys. 73(7), 1980) in the case of Raman scattering, and in many other experimental works. In this paper, we investigate the emission of a fluorescent dye analytically, using the electric dyadic Green's function in a semiclassical electrodynamic model accounting for the nanosphere scattering, which is evaluated according to Mie theory. The dye is modeled as a dipole, illuminated by an incident wave and the one from the nearby nanosphere. We compare our results with previous ones, based on different approximations. More specifically, assuming the dipolar dye is located beside the NP, we analyze when the latter, in turn, modifies the dye dipole moment since the dye has a certain polarizability and hence responds to the local electric field. We report when this contribution is important for the determination of the dye emission rate and scattering. We use the Lorentzian oscillator model for calculating the polarizability of the dye and investigate excitation rate enhancements in various cases. As results show when the polarizability of the dye becomes comparable to that of the plasmonic nanosphere we have to consider the change in the dipole moment of the dye, as in our electrocynamic model.
只提供摘要形式。通过将发射偶极子定位在谐振纳米球附近,可以实现对偶极子散射的增强。在这项研究中,偶极子代表荧光染料或发射量子点,纳米球在光学频率上表现出等离子共振。已经多次证明,纳米球的存在对偶极子的激发和发射有很大的影响。例如在J. Gersten, A. Nitzan, J. Chem。物理学,73(7),1980)在拉曼散射的情况下,以及在许多其他实验工作。本文利用考虑纳米球散射的半经典电动力学模型中的电并矢格林函数,对荧光染料的发射进行了分析研究,并根据Mie理论对其进行了评价。染料被模拟成偶极子,由入射波和附近纳米球的入射波照射。我们根据不同的近似值,将我们的结果与以前的结果进行比较。更具体地说,假设偶极染料位于NP旁边,由于染料具有一定的极化率,因此对局部电场做出响应,因此我们分析了NP何时反过来改变染料偶极矩。当这一贡献对染料发射率和散射的测定有重要意义时,我们进行了报告。我们使用洛伦兹振荡模型来计算染料的极化率,并研究了各种情况下激发率的增强。结果表明,当染料的极化率与等离子纳米球相当时,我们必须考虑染料偶极矩的变化,就像我们的电动力学模型一样。