The total spontaneous emission rate of a quantum emitter in the presence ofan infinite MoS\textsubscript{2} monolayer is enhanced by several orders ofmagnitude, compared to its free-space value, due to the excitation of surfaceexciton polariton modes and lossy modes. The spectral and distance dependenceof the spontaneous emission rate are analyzed and the lossy-surface-wave,surface exciton polariton mode and radiative contributions are identified. Thetransverse magnetic and transverse electric exciton polariton modes can beexcited for different emission frequencies of the quantum emitter, and theircontributions to the total spontaneous emission rate are different. Tocalculate these different decay rates, we use the non-Hermitian description oflight-matter interactions, employing a Green's tensor formalism. The distancedependence follows different trends depending on the emission energy of quantumemitter. For the case of the lossy surface waves, the distance dependencefollows a $z^{-n}$, $n=2,3,4$, trend. When transverse magnetic excitonpolariton modes are excited, they dominate and characterize the distancedependence of the spontaneous emission rate of a quantum emitter in thepresence of the MoS\textsubscript{2} layers. The interaction between a quantumemitter and a MoS\textsubscript{2} superlattice is investigated and we observea splitting of the modes supported by the superlattice. Moreover, a blue shiftof the peak values of the spontaneous emission rate of a quantum emitter isobserved as the number of layers is increased. The field distribution profiles,created by a quantum emitter, are used to explain this behavior.
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机译:由于表面激子极化模式和有损模式的激发,在无限的MoS \ textsubscript {2}单层存在下,量子发射器的总自发发射速率与其自由空间值相比增加了几个数量级。分析了自发发射率的光谱和距离依赖性,并确定了有损表面波,表面激子极化模式和辐射贡献。对于不同的量子发射器发射频率,可以激发出横向的激子和横向的激子极化模式,它们对总自发发射率的贡献是不同的。为了计算这些不同的衰减率,我们使用格林的张量形式主义使用光的相互作用的非赫米特描述。距离依赖性遵循不同的趋势,这取决于量子发射体的发射能量。对于有损表面波,距离依赖性遵循$ z ^ {-n} $,$ n = 2,3,4 $趋势。当横向磁激子极化模式被激发时,它们在MoS \ textsubscript {2}层的存在下占主导地位,并表征了量子发射器自发发射速率的距离依赖性。研究了量子发射体和MoS \ textsubscript {2}超晶格之间的相互作用,我们观察到超晶格支持的模式的分裂。而且,随着层数的增加,观察到了量子发射器的自发发射率的峰值的蓝移。由量子发射器创建的场分布轮廓用于解释这种行为。
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