Polarization-Independent Guided-Mode Resonance Filters under Oblique Incidence

We present the dispersion relation of guided-mode resonances in planar periodic waveguides, both for s-polarized （TF, mode） and p-polarized （TM mode） incident waves. For a fixed homogeneous planar waveguide, dispersion curves of the TE eigenmode cannot cross that of the TM eigenmode at all. That is to say, at a certain wavelength, TE and TM modes cannot be excited with the same propagation constant. Due to Bragg reflection in the planar periodic waveguide, dispersion curves of the TE leaky mode may intersect with that of the TM leaky mode in the first Brillouin zone. We employ these intersections to achieve polarization-independent guided-mode resonance filters.     

电光效应的自相似性

通过对KNbO₃,LiNbO₃,BaTiO₃及几种半导体晶体的电光系数进行数值分析，发现电光系数在自由状态和受夹状态下对应的Miller-δ系数相同，与外加电场频率无关，进而提出用Miller-δ系数表征晶体非线性光学性质.在此基础上，提出一种全新的电光效应产生机制，认为电光效应源于非线性系统的自相似性，表现为对线性性质的一种“自我复制”，而Miller-δ系数是“自我复制”的比例因子. 关键词： 电光效应 非线性光学 自相似性     

声光衍射下He-Ne激光光强分布实验探讨

论文介绍了声光衍射的分类,概述了He-Ne激光在拉曼-奈斯声光衍射下光强分布的实验过程,探讨了声光衍射下He-Ne激光光强分布的特点及实验意义等.     

Na_3AlF_6-AlF_3熔盐中Ti(Ⅳ)的阴极还原机理

应用循环伏安法和计时电位法研究了在990℃下Na3AlF6-AlF3熔盐中,TiO2钨丝电极上的阴极还原机理.实验表明,Ti(Ⅳ)电沉积过程分两步进行:即首先是Ti(Ⅳ)还原为Ti(Ⅱ),然后Ti(Ⅱ)再还原为金属钛,可表示为:Ti(Ⅳ)→Ti(Ⅱ)→Ti.