Yadav Ravindra Kumar, Bourgeois Marc R, Cherqui Charles, Juarez Xitlali G, Wang Weijia, Odom Teri W, Schatz George C, Basu Jaydeep Kumar
Department of Physics, Indian Institute of Science, Bangalore 560 012, India.
Department of Chemistry, Northwestern University, Evanston, Illinois 60208, United States.
ACS Nano. 2020 Jun 23;14(6):7347-7357. doi: 10.1021/acsnano.0c02785. Epub 2020 Jun 2.
Colloidal quantum dot (CQD) assemblies exhibit interesting optoelectronic properties when coupled to optical resonators ranging from Purcell-enhanced emission to the emergence of hybrid electronic and photonic polariton states in the weak and strong coupling limits, respectively. Here, experiments exploring the weak-to-strong coupling transition in CQD-plasmonic lattice hybrid devices at room temperature are presented for varying CQD concentrations. To interpret these results, generalized retarded Fano-Anderson and effective medium models are developed. Individual CQDs are found to interact locally with the lattice yielding Purcell-enhanced emission. At high CQD densities, polariton states emerge as two-peak structures in the photoluminescence, with a third polariton peak, due to collective CQD emission, appearing at still higher CQD concentrations. Our results demonstrate that CQD-lattice plasmon devices represent a highly flexible platform for the manipulation of collective spontaneous emission using lattice plasmons, which could find applications in optoelectronics, ultrafast optical switches, and quantum information science.
当胶体量子点(CQD)组件与光学谐振器耦合时,会展现出有趣的光电特性,分别在弱耦合和强耦合极限下,从珀塞尔增强发射到混合电子和光子极化激元态的出现。在此,针对不同的CQD浓度,展示了在室温下探索CQD - 等离子体晶格混合器件中从弱耦合到强耦合转变的实验。为了解释这些结果,开发了广义延迟法诺 - 安德森模型和有效介质模型。发现单个CQD与晶格发生局部相互作用,产生珀塞尔增强发射。在高CQD密度下,极化激元态在光致发光中呈现为双峰结构,由于集体CQD发射,在更高的CQD浓度下会出现第三个极化激元峰。我们的结果表明,CQD - 晶格等离子体器件是利用晶格等离子体操纵集体自发发射的高度灵活平台,可应用于光电子学、超快光开关和量子信息科学领域。