非线性光学中体积和表面现象的积分方程方法和消光定理

A. V. Ghiner, G. Surdutovich
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引用次数: 0

摘要

分子光学积分方程方法[1]是将介质表示为离散振子系统,在从微观场到宏观场的过程中,不使用平均运算,对介质中的电磁现象进行自洽描述。[2]在局部(微观)场概念的限制下,尝试将积分方程方法应用于非线性光学。为了证明非线性极化满足波动方程这一基本假设的正确性,有必要假设相当严格的限制条件——平面泵浦波、介质间的平面界面、给定场的近似等。在文献[3]中,这一问题是在一般情况下解决的,没有上述假设,但只针对具有非线性偶极机制的非磁性介质。
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Method of integral equations and extinction theorem in volumetric and surface phenomena in nonlinear optics
The method of integral equations of molecular optics [1] is based on the representation of the medium as the system of discrete oscillators and gives self-consistent description of the electromagnetic phenomena in medium without using operation of averaging when one comes from micro to macro-scopic field. In [2] the attempt has been made to apply method of integral equations to the nonlinear optics within the limits of the conception of local (microscopic) field. For justification of the corner-stone assumption that non-lineal polarization satisfies the wave equation it is necessary to assume the number of rather strict restrictions — plane pumping wave, plane interface between the media, approximation of given field and so on. In [3] this problem was solved in a general case without the above-mentioned assumptions but only for nonmagnetic medium with dipole mechanism of nonlinearity.
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