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多发射器的少模场量子化

Few-mode field quantization for multiple emitters.

作者信息

Sánchez-Barquilla Mónica, García-Vidal Francisco J, Fernández-Domínguez Antonio I, Feist Johannes

机构信息

Departamento de Física Teórica de la Materia Condensada and Condensed Matter Physics Center (IFIMAC), Universidad Autónoma de Madrid, E-28049 Madrid, Spain.

Institute of High Performance Computing, Agency for Science, Technology, and Research (ASTAR), Connexis, 138632 Singapore, Singapore.

出版信息

Nanophotonics. 2022 Aug 22;11(19):4363-4374. doi: 10.1515/nanoph-2021-0795. eCollection 2022 Sep.

DOI:10.1515/nanoph-2021-0795
PMID:36147197
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9455278/
Abstract

The control of the interaction between quantum emitters using nanophotonic structures holds great promise for quantum technology applications, while its theoretical description for complex nanostructures is a highly demanding task as the electromagnetic (EM) modes form a high-dimensional continuum. We here introduce an approach that permits a quantized description of the full EM field through a small number of discrete modes. This extends the previous work in ref. (I. Medina, F. J. García-Vidal, A. I. Fernández-Domínguez, and J. Feist, "Few-mode field quantization of arbitrary electromagnetic spectral densities," , vol. 126, p. 093601, 2021) to the case of an arbitrary number of emitters, without any restrictions on the emitter level structure or dipole operators. The low computational demand of this method makes it suitable for studying dynamics for a wide range of parameters. We illustrate the power of our approach for a system of three emitters placed within a hybrid metallodielectric photonic structure and show that excitation transfer is highly sensitive to the properties of the hybrid photonic-plasmonic modes.

摘要

利用纳米光子结构控制量子发射器之间的相互作用,在量子技术应用方面具有巨大潜力,而对于复杂纳米结构,其理论描述是一项极具挑战性的任务,因为电磁(EM)模式构成了一个高维连续体。我们在此介绍一种方法,该方法允许通过少量离散模式对全EM场进行量子化描述。这将参考文献(I. Medina、F. J. García-Vidal、A. I. Fernández-Domínguez和J. Feist,“任意电磁谱密度的少模场量子化”,第126卷,第093601页,2021年)中先前的工作扩展到任意数量发射器的情况,对发射器能级结构或偶极算符没有任何限制。该方法的低计算需求使其适用于研究各种参数下的动力学。我们展示了我们的方法对于置于混合金属 - 电介质光子结构中的三个发射器系统的强大功能,并表明激发转移对混合光子 - 等离子体模式的性质高度敏感。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/29631ec3f829/j_nanoph-2021-0795_fig_005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/e2bbc3a13d85/j_nanoph-2021-0795_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/fe524d31321c/j_nanoph-2021-0795_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/267dd5e9f4ef/j_nanoph-2021-0795_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/189691c730a7/j_nanoph-2021-0795_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/29631ec3f829/j_nanoph-2021-0795_fig_005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/e2bbc3a13d85/j_nanoph-2021-0795_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/fe524d31321c/j_nanoph-2021-0795_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/267dd5e9f4ef/j_nanoph-2021-0795_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/189691c730a7/j_nanoph-2021-0795_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d0b3/11501957/29631ec3f829/j_nanoph-2021-0795_fig_005.jpg

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