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激子 - 等离子体能量交换驱动向强耦合 regime 的转变。 (注:这里“regime”可根据具体语境灵活翻译,比如“状态”“ regime”等,因未明确更合适的中文释义,暂保留英文)

Exciton-Plasmon Energy Exchange Drives the Transition to a Strong Coupling Regime.

作者信息

Shahbazyan Tigran V

机构信息

Department of Physics , Jackson State University , Jackson , Mississippi 39217 , United States.

出版信息

Nano Lett. 2019 May 8;19(5):3273-3279. doi: 10.1021/acs.nanolett.9b00827. Epub 2019 Apr 17.

Abstract

We present a model for exciton-plasmon coupling based on an energy exchange mechanism between quantum emitters (QE) and localized surface plasmons in metal-dielectric structures. Plasmonic correlations between QEs give rise to a collective state exchanging its energy cooperatively with a resonant plasmon mode. By defining carefully the plasmon mode volume for a QE ensemble, we obtain a relation between QE-plasmon coupling and a cooperative energy transfer rate that is expressed in terms of local fields. For a single QE near a sharp metal tip, we find analytically the enhancement factor for QE-plasmon coupling relative to QE coupling to a cavity mode. For QEs distributed in an extended region enclosing a plasmonic structure, we find that the ensemble QE-plasmon coupling saturates to a universal value independent of system size and shape, consistent with the experiment.

摘要

我们提出了一种基于量子发射器(QE)与金属-电介质结构中的局域表面等离子体激元之间能量交换机制的激子-等离子体激元耦合模型。量子发射器之间的等离子体激元相关性产生了一种集体态,该集体态与共振等离子体激元模式协同交换能量。通过仔细定义量子发射器系综的等离子体激元模式体积,我们得到了量子发射器-等离子体激元耦合与以局部场表示的协同能量转移速率之间的关系。对于尖锐金属尖端附近的单个量子发射器,我们通过解析得到了量子发射器-等离子体激元耦合相对于量子发射器与腔模耦合的增强因子。对于分布在包围等离子体激元结构的扩展区域中的量子发射器,我们发现系综量子发射器-等离子体激元耦合饱和到一个与系统尺寸和形状无关的通用值,这与实验结果一致。

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