双折射吸收非线性介质薄膜中倍频的产生  

Second-harmonic power generated in the absorbing and birefringent nonlinear medium

作　　者：颜国君[1] 陈光德[1] 伍叶龙[1] 杨建清[1] 

机构地区：[1]西安交通大学理学院应用物理系,西安710049

出　　处：《物理学报》2008年第1期265-270,共6页Acta Physica Sinica

摘　　要：从二次谐波电场满足的波动方程出发,考虑到介质对二次谐波的吸收以及把完全边界条件应用于基频波和二次谐波在介质的入射面和出射面之间的反射效应,推导出了单光轴非线性薄膜介质中的二次谐波输出功率的计算式.结果表明:当采用复折射率的概念时,可以把非线性无吸收介质的二次谐波输出功率计算式应用到非线性吸收介质二次谐波输出功率计算式中去.Considering the absorption of the nonlinear medium to the second-harmonic （SH） wave and using the complete boundary conditions for the reflections of the fundamental and SH waves at the input and output faces of the nonlinear medium, a formula for calculating the second-harmonic power generated in the absorbing and birefringent nonlinear medium was derived from the Maxwell＇s equation that the SH field E2 satisfies. The result shows that the formula for calculating the second-harmonic power generated in the nonzero absorption medium can be used for calculating the second-harmonic power generated in the absorptive medium if the complex refractive index, instead of the ordinary refractive index is used.

关 键 词：非线性 倍频 二次谐波功率 

分 类 号：TN25[电子电信—物理电子学]