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一种新型优质光子晶体偏振滤波器的设计 总被引:4,自引:1,他引:3
设计了一种各向异性的一维掺杂光子晶体,利用特征矩阵法研究了该各向异性一维掺杂光子晶体的偏振滤波特性,并与各向同性的一维掺杂光子晶体的两个偏振态缺陷模进行了比较.结果表明,当光以不同角度入射时,透射波中横电波(TE)和横磁波(TM)的缺陷模都会出现明显的分离.利用这个特性设计出一种新型优质光子晶体偏振滤波器. 相似文献
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采用一维介电体系中处理光传播的方法—传输矩阵法,详细推导了含有缺陷层的异质镜像光子晶体(ABCCBA)PD(ABCCBA)Q中透射率的计算公式,并用Matlab编程模拟了异质三周期镜像光子晶体中无缺陷层和引入缺陷层D时,光子带隙的数目和带宽及缺陷模的数目和透射率随缺陷层位置、厚度、介质周期数的变化情况。模拟结果表明:对于此结构的光子晶体,当缺陷层位于中央位置、周期数N=8、10,厚度变化且为某些特定值时,其光子带隙数目、缺陷模数目及透射率有最佳值。这一研究为设计可调谐滤波器、多通道滤波器提供了重要的理论基础。 相似文献
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基于磁流体的折射率对外加变化磁场的敏感特性,提出将磁流体作为缺陷层引入到一维光子晶体中实现磁场传感。由于缺陷的存在,使得光子晶体的透射谱中产生缺陷峰。该传感器可通过测量磁场变化时光子晶体缺陷模波长的移动对相应的磁场进行测量。利用传输矩阵法对不同结构参数下,缺陷模波长随在外加磁场的变化进行了模拟计算,为实际磁场传感器的设计提供了理论参考。 相似文献
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本文提出了负折射率缺陷层的一维各向异性光子晶体结构,利用传输矩阵的方法给出了TE波和TM波的透射率,结果表明在TE波中出现两个及多个缺陷模,TM波存在单缺陷模,两种偏振状态不同的透射波的缺陷模能分开,得出了光通过负折射率缺陷层的一维各向异性光子晶体后TE波和TM波随入射角的变化特性、随缺陷层厚度的的变化特性。这些特性用于光子晶体多通滤波、光子晶体偏振和激光谐振腔等器件的设计具有重要意义。 相似文献
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杂质吸收对一维光子晶体缺陷模的影响 总被引:11,自引:1,他引:11
为了研究杂质吸收对一维光子晶体缺陷模的影响,采用复折射率和法布里-珀罗(F-P)干涉法,计算出掺有吸收杂质的一维光子晶体的缺陷模透射率和反射率随消光系数的变化特征。得出消光系数对一维掺杂光子晶体的缺陷模的透射率和反射率会产生显著的影响。当消光系数由0增加到0.03时缺陷模的透射率由1减少为0。当消光系数由0增加到0.03时缺陷模的反射率由0增加到0.86。消光系数增加时反射波中的缺陷模宽度会增大,而消光系数的变化对透射波中的缺陷模宽度影响很小。 相似文献
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A magneto-photonic crystal (MPC) is defined as a periodic light-guided structure involving magnetic materials or a photo- nic crystal with some magnetic-material defects. The transfer matrices of guided optical waves (GOWs) propagating re- spectively in magneto-optical and non-magnetic dielectric layers are deduced according to the coupled-mode theory. The transmission spectra of GOWs in one-dimensional magneto-photonic crystals (1 D-MPC) are investigated by the transfer matrix method. It is shown that the two sharp peaks in the 1D-MPC's transmission spectra can be used for high-resolution magnetic field sensing; and a comb filter with six channels can be achieved by optimizing the 1D-MPC structure and controlling the external magnetic field. 相似文献
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The interaction of electromagnetic radiation with a time-switched magnetoplasma is considered. It is shown that for longitudinal propagation within the so-called radio approximation (neglecting ion motion), the original wave splits into three waves whose frequencies are different from that of the incident wave. One of the waves is strongly influenced by the static magnetic field, and its frequency can be controlled by the strength of this field. Numerical results are presented for the cases of right-hand and left-hand circular polarization of the incident waves 相似文献
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《Microwave Theory and Techniques》1967,15(1):37-41
A nonreciprocal circular polarizer has been developed. This ferrite device converts linear polarization propagating in rectangular waveguide into circular polarization propagating in circular waveguide. The sense, right- or left-hand, of the circular polarization is determined by the direction of a longitudinal magnetic field applied to the ferrite. If one sense of circular polarization, e.g., right-hand, is transmitted, then only left-hand circuIar polarization can be received. Performance data indicate good ellipticity with reasonable loss and VSWR for two models of the circular polarizer, and for two devices--a circulator and a nonreciprocal antenna element--based on the polarizer. The antenna element permits one antenna to be used both to transmit and to receive the reflected circularly polarized signals from a target. 相似文献
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A tunable photonic crystal (PC) filter is proposed with the twisted nematic (TN) liquid crystal (LC) as a defect layer. The
polarization sensitive performance and the eigenmodes are analyzed. The results show that there are two kinds of transmission
modes, namely o and e, when the voltage is low. The different modes can be selected by rotating the filter axially. The e
mode shifts toward the shorter wavelength side as the applied voltage increases. Then the peaks of two modes merge into each
other and the polarization sensitive performance disappears. The photonic band gap is insensitive to the voltage. The tunable
range of the filter is 53 nm. 相似文献
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通过对设计出的一维掺杂光子晶体的数值计算和理论分析,得出了两个偏振态缺陷模的透射峰的变化特征为:TM波其缺陷模透射峰在入射角大于0.75(rad)范围内有多条明显的缺陷模透射峰带,而TE波在入射角大于0.75(rad) 范围内没有缺陷模透射峰;TM波缺陷模透射峰的波长 随杂质光学厚度 近似呈线性变化,并且同一空气膜厚度值可以截到两个波长不同的透射峰。以此为基础设计出:滤波通道波长可调范围大于100nm 、滤波通道的半高宽可调范围在1 nm — 6nm、滤波通道透射峰值大于0.98的一维光子晶体双通道可调谐偏振滤波器。 相似文献