共查询到19条相似文献,搜索用时 93 毫秒
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两类单负材料组成的一维半无限光子晶体反射谱 总被引:1,自引:1,他引:0
运用传输矩阵方法和Bloch定理计算了两类单负材料组成的一维半无限光子晶体反射谱,与有限多层结构通带中振荡的反射谱相比,半无限结构的反射谱曲线是光滑的,是有限周期结构反射谱振幅取平均的结果,可用来估计通带中的反射率.研究半无限结构的反射谱,有利于分析带隙的位置和宽度,结果表明,由两类单负材料组成的光子晶体中,不仅存在零有效位相带隙,还存在角度带隙,尤其发现高频处的Bragg带隙也是一个全方位带隙. 相似文献
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等离子体光子晶体是等离子体和介质(真空)构成的人工周期性结构.用分段线性电流密度 递归卷积时域有限差分(PLCDRC-FDTD)算法分析了等离子体光子晶体和缺陷等离子体光子 晶体.从时域的角度分析了高斯脉冲在等离子体光子晶体中的传播过程,给出了时域反射和 透射波形.然后,从频域的角度分析了等离子体光子晶体和带缺陷的等离子体光子晶体的电 磁反射系数和透射系数.计算表明,等离子体光子晶体对频率小于等离子体频率的低频电磁 波几乎完全反射,而透射的电磁波则为频率高于等离子体频率的电磁波.在高频,等离子体 光子晶体则出现类似一般光子晶体的光子带隙特性.
关键词:
等离子体
光子晶体
时域有限差分法
等离子体光子晶体 相似文献
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应用多光子非线性Compton散射模型和时域有限差分法,对多光子非线性Compton散射对非均匀等离子体光子晶体光子带隙特性的影响进行了研究,提出将入射和散射光作为形成光子带隙的新机制,对电磁波方程进行了修正.结果表明:与Compton散射前相比,散射使电磁波幅值衰减更快|随等离子体密度增加,透射谱禁带宽度几乎无变化,其中心频率向高频方向有明显移动,向上的峰值有较大增加,反射谱向下的峰值有明显减小|随温度增加,透射谱禁带宽明显减小,向上的峰值略有减小,透射能量有所降低|随两种介质介电系数比增加,光子禁带数增加,且带隙间距显著减小. 相似文献
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基于对光纤传输特性和胶体光子晶体制备方法的研究,提出了用外加电场控制的方法制备光子带隙位于通讯波段的FCC结构的胶体光子晶体,并用光纤系统测试胶体光子晶体的带隙特性.采用RSOFT模拟了胶体光子晶体的带隙,分析了带隙位于通讯波段时所需的胶体微球的基本参量(微球折射率和直径).采用自组装的方法,用步进电机控制玻璃基片向上的拉升速率.速率为5 μm/s,同时外加一电场.用扫描电镜观测胶体晶体的表面形貌,并设计了单模光纤系统测量胶体光子晶体的带隙特性.测试的透射谱线表明胶体光子晶体的带隙中心波长为1552 nm.测试结果和模拟结果具有很好的一致性,误差只有2 nm. 相似文献
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利用传输矩阵法对太赫兹自由电子激光光腔光子晶体镜进行了模拟设计,中心波段在1~3 THz。对光腔镜的光子晶体结构参数如介质厚度、层数、折射率与反射率的关系等进行了研究,并给出了一维光子晶体用于高反镜的设计方法。通过对耦合输出镜光子晶体中引入缺陷层情况的数值模拟,发现通过对缺陷层的调节设计,可以实现耦合输出率的可调谐;并给出了可用于THz 自由电子激光光腔耦合输出镜的调节方法。通过对介质层厚度的调节设计,可以实现反射光谱的整体移动,从而实现宽谱可调谐,扩大了高反镜及耦合输出镜的调节范围。 相似文献
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利用有限元法和传输矩阵法,对柚子型结构的光子晶体光纤啁啾光栅的反射谱进行了理论分析。得到了啁啾光栅参数和光纤参数对光子晶体光纤啁啾光栅反射谱的影响规律。结果表明随着啁啾系数和折变量的增加,光栅反射谱呈规律变化,当啁啾系数增大到一定程度时几个反射峰会连到一起,形成一个大的反射带宽。光纤的内包层直径和纤芯直径的改变能够影响各反射峰之间的间距。同时研究了切趾变迹对光子晶体光纤啁啾光栅反射谱的影响,研究表明,所用切趾函数会同时对多个峰进行切趾,每个峰的切趾效果都很好。对反射谱波动较大的几个峰相连的啁啾光栅经过柯西切趾后反射谱曲线平滑,适合于实际应用。 相似文献
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Galina V. Li Ekaterina V. Astrova Sergey A. Dyakov Anna Baldycheva Tatiana S. Perova Sergey G. Tikhodeev Nikolay A. Gippius 《固体物理学:研究快报》2013,7(7):481-484
The reflection and transmission spectra of a finite thickness 2D photonic crystal slab (PCS) based on macroporous silicon are investigated. Periodic photonic crystal region is separated from air by homogeneous silicon interfacial layers. These interfacial layers at the silicon/air boundary being defects of the photonic crystal lattice, define the properties of surface Tamm states in the photonic stop‐bands (PSBs). It is demonstrated experimentally and theoretically that the reflection spectra of a structure with different thicknesses of the interfacial layers on both sides of the PCS depend on the illuminated side. At the same time, the transmission spectra are identical for both light directions in agreement with the reciprocity principle. Analysis shows that the dependence of the reflection spectrum on the side of light entrance is due to scattering losses in the real structure. (© 2013 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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A novel technique is used to measure the concentration of glycerol in blood-hemoglobin-glycerol (B–H–G) solution using 3D photonic crystal structure is presented in this paper. Glycerol concentration is estimated accurately by measuring the intensities of transmitted light. Here, reflection as well as absorption losses is considered to measure the transmitted intensity of light having wavelength 540 nm. The principle of measurement is based on the linear variation of photonic band gap with respect to glycerol concentration. Simulations for photonic band gap are made using plane wave expansion (PWE) method. An experimental set up is theoretically designed to measure the concentration of glycerol at different hemoglobin concentration. 相似文献
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Plasmonic waveguides and conventional dielectric waveguides have favorable characteristics in photonic integrated circuits. Typically, plasmonic waveguides can provide subwavelength mode confinement, as shown by their small mode area, whereas conventional dielectric waveguides guide light with low loss, as shown by their long propagation length. However, the simultaneous achievement of subwavelength mode confinement and low-loss propagation remains limited. In this paper, we propose a novel design of an alldielectric bowtie waveguide, which simultaneously exhibits both subwavelength mode confinement and theoretically lossless propagation. Contrary to traditional dielectric waveguides, where the guidance of light is based on total internal reflection, the principle of the all-dielectric bowtie waveguide is based on the combined use of the conservation of the normal component of the electric displacement and the tangential component of the electric field, such that it can achieve a mode area comparable to its plasmonic counterparts. The mode distribution in the all-dielectric bowtie waveguide can be precisely controlled by manipulating the geometric design. Our work shows that it is possible to achieve extreme light confinement by using dielectric instead of lossy metals. 相似文献
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Shaobin Liu Wei Hong Naichang Yuan 《International Journal of Infrared and Millimeter Waves》2006,27(3):403-423
The plasma photonic crystal is a periodic array composed of alternating thin unmagnetized (or magnetized) plasmas and dielectric
materials (or vacuum). In this paper, the piecewise linear current density recursive convolution finite-difference time-domain
method for the simulation of isotropic unmagnetized plasma is applied to model unmagnetized plasma photonic crystal structures.
A perfectly matched layer absorbing material is used in these simulations. In time-domain, the electromagnetic propagation
process of a Gaussian pulse through an unmagnetized plasma photonic crystal is investigated. In frequency-domain, the reflection
and transmission coefficients through unmagnetized plasma photonic crystals are computed and their dependence on plasma frequency,
plasma thickness, collision frequency is studied. The results show theoretically that the electromagnetic bandgaps of unmagnetized
plasma photonic crystals are tuned by the plasma parameters. 相似文献