Mishchenko Michael I
NASA Goddard Institute for Space Studies, 2880 Broadway, New York, NY 10025, USA.
J Quant Spectrosc Radiat Transf. 2017 Oct;200:137-145. doi: 10.1016/j.jqsrt.2017.06.003. Epub 2017 Jun 13.
The majority of previous studies of the interaction of individual particles and multi-particle groups with electromagnetic field have focused on either elastic scattering in the presence of an external field or self-emission of electromagnetic radiation. In this paper we apply semi-classical fluctuational electrodynamics to address the ubiquitous scenario wherein a fixed particle or a fixed multi-particle group is exposed to an external quasi-polychromatic electromagnetic field as well as thermally emits its own electromagnetic radiation. We summarize the main relevant axioms of fluctuational electrodynamics, formulate in maximally rigorous mathematical terms the general scattering-emission problem for a fixed object, and derive such fundamental corollaries as the scattering-emission volume integral equation, the Lippmann-Schwinger equation for the dyadic transition operator, the multi-particle scattering-emission equations, and the far-field limit. We show that in the framework of fluctuational electrodynamics, the computation of the self-emitted component of the total field is completely separated from that of the elastically scattered field. The same is true of the computation of the emitted and elastically scattered components of quadratic/bilinear forms in the total electromagnetic field. These results pave the way to the practical computation of relevant optical observables.
以往关于单个粒子和多粒子组与电磁场相互作用的大多数研究,要么聚焦于存在外场时的弹性散射,要么聚焦于电磁辐射的自发射。在本文中,我们应用半经典涨落电动力学来处理一种普遍存在的情形,即一个固定粒子或一个固定多粒子组受到外部准多色电磁场作用,同时热发射自身的电磁辐射。我们总结了涨落电动力学的主要相关公理,以最严格的数学形式表述了固定物体的一般散射 - 发射问题,并推导了诸如散射 - 发射体积积分方程、并矢跃迁算符的 Lippmann - Schwinger 方程、多粒子散射 - 发射方程以及远场极限等基本推论。我们表明,在涨落电动力学框架下,总场自发射分量的计算与弹性散射场的计算完全分离。总电磁场中二次/双线性形式的发射分量和弹性散射分量的计算也是如此。这些结果为相关光学可观测量的实际计算铺平了道路。