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在非线性等离子体腔中,激子-等离子体激元极化激元态促进的简并参量下转换。

Degenerate parametric down-conversion facilitated by exciton-plasmon polariton states in a nonlinear plasmonic cavity.

机构信息

Theoretical Division, Los Alamos National Laboratory, Los Alamos, NM 87545, United States of America.

Department of Physics, Arizona State University, Tempe, AZ 85287, United States of America.

出版信息

Nanotechnology. 2023 Feb 10;34(17). doi: 10.1088/1361-6528/acb5a8.

Abstract

We study the effect of degenerate parametric down-conversion (DPDC) in an ensemble of two-level quantum emitters (QEs) coupled via near-field interactions to a single surface plasmon (SP) mode of a nonlinear plasmonic cavity. For this purpose, we develop a quantum driven-dissipative model capturing non-equilibrium dynamics of the system in which incoherently pumped QEs have transition frequency tuned near the second-harmonic response of the SPs. Considering the strong coupling regime, i.e. the SP-QE interaction rate exceeds system dissipation rates, we find a critical SP-QE coupling attributed to the phase transition between normal and lasing steady states. Examining fluctuations above the system's steady states, we predict new elementary excitations, namely, the exciton-plasmon polaritons formed by the two-SP quanta and single-exciton states of QEs. The contribution of two-SP quanta results in the linear scaling of the SP-QE interaction rate with the number of QEs,o, as opposed to theo-scaling known for the Dicke and Tavis-Cummings models. We further examine how SP-QE interaction scaling affects the polariton dispersions and power spectra in the vicinity of the critical coupling. For this purpose, we compare the calculation results assuming a finite ensemble of QEs and the model thermodynamic limit. The calculated power spectra predict an interplay of coherent photon emission by QEs near the second-harmonic frequency and correlated photon-pair emission at the fundamental frequency by the SPs (i.e. the photonic DPDC effect).

摘要

我们研究了通过近场相互作用耦合到非线性等离子体腔的单个表面等离子体(SP)模式的两个能级量子发射器(QE)的简并参量下转换(DPDC)的影响。为此,我们开发了一个量子驱动耗散模型,该模型捕获了系统的非平衡动力学,其中非相干泵浦 QE 的跃迁频率调谐到 SP 的二次谐波响应附近。考虑到强耦合状态,即 SP-QE 相互作用速率超过系统耗散速率,我们发现了一个临界 SP-QE 耦合,归因于正常和激光稳态之间的相变。检查系统稳态以上的波动,我们预测了新的基本激发,即由两个 SP 量子和 QE 的单激子态形成的激子-等离子体极化激元。两个 SP 量子的贡献导致 SP-QE 相互作用速率与 QE 的数量呈线性比例关系,o,与众所周知的 Dicke 和 Tavis-Cummings 模型的o 比例关系相反。我们进一步研究了 SP-QE 相互作用比例如何影响临近临界耦合的极化激元色散和功率谱。为此,我们比较了在有限的 QE 集合和模型热力学极限下的计算结果。计算出的功率谱预测了 QE 在二次谐波频率附近的相干光子发射和 SP 在基频处的相关光子对发射(即光子 DPDC 效应)之间的相互作用。

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