Wen Sha-Sha, Huang Yong-Gang, Wang Xiao-Yun, Liu Jie, Li Yun, Quan Xiu-E, Yang Hong, Peng Jin-Zhang, Deng Ke, Zhao He-Ping
Opt Express. 2020 Mar 2;28(5):6469-6489. doi: 10.1364/OE.386828.
A bound state between a quantum emitter (QE) and surface plasmon polaritons (SPPs) can be formed, where the excited QE will not relax completely to its ground state and is partially stabilized in its excited state after a long time. We develop some theoretical methods for investigating this problem and show how to form such a bound state and its effect on the non-Markovian decay dynamics. We put forward an efficient numerical approach for calculating the analytical part of the self-energy for frequency below the lower energy threshold. We also propose an efficient formalism for obtaining the long-time value of the excited-state population without calculating the eigenfrequency of the bound state or performing a time evolution of the system, in which the probability amplitude for the excited state in the steady limit is equal to one minus the integral of the evolution spectrum over the positive frequency range. With the above two quantities obtained, we show that the non-Markovian decay dynamics of an initially excited QE can be efficiently obtained by the method based on the Green's function expression for the evolution operator when a bound state exists. A general criterion for identifying the existence of a bound state is presented. The performances of the above methods are numerically demonstrated for a QE located around a metal nanosphere and in a gap plasmonic nanocavity. Numerical results show that these methods work well and the QE becomes partially stabilized in its excited state at a long time for the transition dipole moment beyond its critical value. In addition, it is also found that this critical value is heavily dependent on the distance between the QE and the metal surface, but nearly independent on the size of the nanosphere or the rod. Our methods can be utilized to understand the suppressed decay dynamics for a QE in an open quantum system and provide a general picture on how to form such a bound state.
量子发射体(QE)与表面等离激元极化激元(SPP)之间可以形成束缚态,其中被激发的QE不会完全弛豫到基态,而是在长时间后部分稳定在激发态。我们开发了一些理论方法来研究这个问题,并展示如何形成这样的束缚态及其对非马尔可夫衰变动力学的影响。我们提出了一种有效的数值方法来计算低于较低能量阈值频率下自能的解析部分。我们还提出了一种有效的形式体系,用于在不计算束缚态本征频率或不对系统进行时间演化的情况下获得激发态布居的长时间值,其中稳态极限下激发态的概率幅等于1减去正频率范围内演化谱的积分。得到上述两个量后,我们表明当存在束缚态时,基于演化算符的格林函数表达式的方法可以有效地获得初始激发的QE的非马尔可夫衰变动力学。提出了识别束缚态存在的一般标准。针对位于金属纳米球周围和间隙等离子体纳米腔中的QE,对上述方法的性能进行了数值演示。数值结果表明这些方法效果良好,对于跃迁偶极矩超过其临界值的情况,QE在长时间后部分稳定在激发态。此外,还发现这个临界值很大程度上取决于QE与金属表面之间的距离,但几乎与纳米球或纳米棒的尺寸无关。我们的方法可用于理解开放量子系统中QE的衰变动力学抑制,并提供关于如何形成这样的束缚态的总体情况。