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A multiple-scattering approach to interatomic interactions and superradiance in inhomogeneous dielectrics

机译:非均匀介电体中原子间相互作用和超辐射的多重散射方法

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摘要

The dynamics of a collection of resonant atoms embedded inside an inhomogeneous nondispersive and lossless dielectric is described with a dipole Hamiltonian that is based on a canonical quantization theory. The dielectric is described macroscopically by a position-dependent dielectric function and the atoms as microscopic harmonic oscillators. We identify and discuss the role of several types of Green tensors that describe the spatio-temporal propagation of field operators. After integrating out the atomic degrees of freedom, a multiple-scattering formalism emerges in which an exact Lippmann-Schwinger equation for the electric field operator plays a central role. The equation describes atoms as point sources and point scatterers for light. First, single-atom properties are calculated such as position-dependent spontaneous-emission rates as well as differential cross sections for elastic scattering and for resonance fluorescence. Secondly, multi-atom processes are studied. It is shown that the medium modifies both the resonant and the static parts of the dipole-dipole interactions. These interatomic interactions may cause the atoms to scatter and emit light cooperatively. Unlike in free space, differences in position-dependent emission rates and radiative line shifts influence cooperative decay in the dielectric. As a generic example, it is shown that near a partially reflecting plane there is a sharp transition from two-atom superradiance to single-atom emission as the atomic positions are varied.
机译:使用偶极哈密顿量描述了嵌入在不均匀,非分散且无损电介质中的共振原子集合的动力学,该偶极哈密顿量基于规范的量化理论。介电层是由位置相关的介电函数宏观描述的,原子是微观谐波振荡器。我们确定并讨论了描述现场算子的时空传播的几种绿色张量的作用。在整合了原子的自由度之后,出现了多重散射形式主义,其中对于电场算子而言,精确的Lippmann-Schwinger方程起着核心作用。该方程式将原子描述为光的点源和点散射体。首先,计算单原子特性,例如位置相关的自发发射率以及弹性散射和共振荧光的微分截面。其次,研究了多原子过程。结果表明,介质改变了偶极-偶极相互作用的共振和静态部分。这些原子间相互作用可能导致原子散射并协同发光。与自由空间不同,与位置有关的发射速率和辐射线位移的差异会影响电介质中的协同衰减。作为一般示例,显示出随着原子位置的变化,在部分反射平面附近,从两原子超辐射到单原子发射有急剧的过渡。

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