Several Steps toward Fundamentals of Physics of Light-Matter Coupling

Rumyantsev
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Abstract

The microscopic theory of optical phenomena in crystals is closely related to the theory of excitons, which provides an appropriate tool for elucidation of specifics of interaction between electromagnetic fields and crystals and for construction of the physical picture of energy transfer in crystalline media. It is well established that in a crystal, where the translation symmetry allows for excitation of any of its elementary cells (or any of the comprising structural units), the energy transfer of electronic excitations occurs due to the motion of quasi-particles called excitons. The concept of “exciton” was originally introduced into physics by the pioneering works of Frenkel [1]. Among the first to consider excitonic states was also Peierls [2]. These works gave a theoretical explanation for the experimentally observed photoelectrically negative light absorption. Utilizing HeitlerLondon-Heisenberg method in his study of electronic states Frenkel [1] demonstrated that the absence of photoconductivity under the light absorption by an electronic subsystem in an ideal crystal stems from excitations of crystalline structural units moving in waves (due to translation invariance) along a crystal. Such excited states were given the name of “Frenkel excitons”.
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迈向光-物质耦合物理学基础的几个步骤
晶体光学现象的微观理论与激子理论密切相关,激子理论为阐明电磁场与晶体相互作用的特性和构建晶体介质中能量传递的物理图景提供了合适的工具。众所周知,在晶体中,平移对称性允许激发其任何基本细胞(或任何组成结构单元),电子激发的能量转移是由于称为激子的准粒子的运动而发生的。“激子”的概念最初是由Frenkel的开创性著作[1]引入物理学的。第一个考虑激子态的人也是Peierls[2]。这些工作为实验观察到的光电负吸收现象提供了理论解释。Frenkel在研究电子态时利用HeitlerLondon-Heisenberg方法[1]证明了理想晶体中电子子系统在光吸收下的光电导率缺失源于晶体结构单元沿晶体以波形式运动(由于平移不变性)的激发。这种激发态被命名为“弗伦克尔激子”。
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