对称单负介质包层平面波导的模式特征

系统研究了负μ材料(MNG)作为包层的对称三层平板波导的传输特性. 研究发现,这种波导既支持快波的传播,又支持TE₀,TE₁模式的慢波传输. 其模式特性不同于左手介质波导和传统介质波导,导模存在的模折射率范围要比它们的大. MNG波导的TE₀快波模缺失,且TE_m模(m>1)的传播常数大于TM_m模的传播常数. TE_m模具有双模特征,且与波导的结构参数密切相关,导致波导中的净能流出现负值. 关键词： 单负介质 平板波导 快波与慢波 传播常数     

有限磁场中等离子体圆柱波导的传播特性

分析了有耗介质中等离子体圆柱波导在有限外加磁场中的传播特性.重点讨论了波导传播常数随等离子体参数、介质参数和外加磁场的变化.分析结果表明，有限强磁场中的等离子体波导的传播特性比无外磁场或外加磁场为无穷大时具有更强的控制能力. 关键词：     

金属包层渐变折射率介质光波导的传输特性与损耗

用金属包层介质光波导损耗的微扰理论及藉助多层近似法用递推公式分析渐变折射率波导传播常数的方法,对几种类型的金属包层渐变折射率介质光波导的传输特性与损耗进行分析和讨论,得到了与精确数值计算结果相吻合的结果.     

部分负曲率太赫兹空芯波导研究

提出了一种新型部分负曲率反谐振空芯太赫兹波导,波导包层包括两部分,一部分由介质圆管组成,为纤芯提供部分负曲率边界;另一部分由多个矩形介质层组成,多介质层可用来降低限制损耗.此波导结构在增加反谐振层的同时不引入新的包层节点,易于实现太赫兹波的宽带低损耗传输.采用全矢量有限元法对波导进行了数值仿真,研究了其宽带低损耗特性.基于此,利用3D打印技术制备了所设计波导,使用太赫兹时域光谱系统对其传输特性进行测试.实验结果表明,该负曲率太赫兹波导在0.29～0.42THz的传输损耗低于10dB/m,与数值仿真结果吻合较好.     

不对称左手介质平板波导模式特性分析

对不对称左手介质平板波导的几个低阶的TE模和TM模进行了数值计算,得到了模式特征方程,分析了归一化传播常数β/k_0随平板厚度d变化的色散关系,作出了模式的电场E_y(x)分布．在左手介质平板波导中,每一模式都有截止点, TE_0模和TM_0模不出现,在我们给出的特定的介质参数下,TE_1模和TM_1模不能和其他高阶模式共存,其归一化传播常数β/ k_0随k_0d的增加而减小．给出的结果对左手介质元器件的研究有实际的参考意义．     

THz波段介质涂敷空芯金属圆波导的传输特性

针对THz波段介质涂敷空芯金属圆波导传输特性的精确分析问题,基于波导中场方程及边界条件建立关于传播常数的特征方程,并且采用改进的Muller法求解特征方程得到涂敷圆波导主模HE11模的传播常数。计算中对THz波段的非理想导体电导率采用经典弛豫效应模型。仿真结果表明:内径为1.8 mm的银波导,当聚苯乙烯涂敷层厚度为17 m时,HE11模在1.5~3.0 THz的衰减常数在1 dB/m以下,且具有较好的色散特性;内径为2.2 mm的银波导,在2.5 THz时其衰减常数随涂敷层厚度的增加先增大后减小,且存在最佳介质涂敷层厚度,可实现THz波低损耗传输。     

负介电常数材料和负磁导率材料的双层结构中电磁波模式分析

研究了双层单负材料结构中电磁波的模式,主要分析了不同模式的产生条件,讨论了这些模式与材料参数之间的关系.当材料参数满足平均介电常数和磁导率为零时出现隧穿模式.当满足波导模产生条件时,波导模式的电磁波在材料两边的半无限真空中以消逝波存在,在双层单负材料的界面处也可以出现较强的局域场. 关键词： 单负材料 传播模式 隧穿模式 波导模式     

光子晶体耦合波导实现光开关效应的研究

提出了一种基于光子晶体耦合波导实现光开关效应的方法:将线缺陷引入二维光子晶体以形成两平行的邻近波导,两邻近波导及其中间的两排介质柱构成了光开关模型耦合区;利用平面波展开法计算了不同介质填充率情况下的色散特性.结果发现:减小介质填充率可以实现波导耦合长度的减小;分段调整中间介质柱的填充率和选择不同的耦合搭配长度,定向耦合...     

基于介质与铁氧体的通阻捷变磁可调频率选择表面设计研究

提出了利用介质陶瓷和铁氧体材料构建可调型带通频率选择表面的设计思路.在C波段波导模式下通过仿真设计出高介电常数方形柱状结构,优化后使其产生宽频的负介电常数,基于等效媒质理论对该结构通阻特性进行分析研究,其传输禁带的产生途径在于介质中产生了具有类Drude谐振形式的电单极子.在相同的仿真环境下对铁氧体结构进行设计优化,调节外加偏置磁场,使铁磁谐振在相应的频点发生,产生负磁导率.利用负介电常数与负磁导率的"双负"特性规律,将两种结构进行组合,协同优化,使电磁谐振相互耦合,实现通带特性.C波段波导模式下的分析表明,两种结构在同一个频点电磁谐振耦合,可以实现"双负"通带的传输效果.在由于铁氧体的磁可调特性,通过改变外加偏置磁场,该通带可以在6—8 GHz范围内可调.对电磁场矢量分布状况和等效参数提取结果进行了数值分析研究,确定了电磁耦合的性质和形成机理,充分验证了这种方法的可行性.对该结构材料样品进行加工,并测试验证,最终实验结果与仿真结果基本一致,实现了"双负"通带的可调.该方法拓展了频率选择表面的设计思路,可用于设计多通带、可调谐频率选择表面.     

线性电介质和中心对称光折变晶体界面表面波的研究

报道了中心对称光折变晶体与线性电介质界面表面波的形成及能量变化. 通过调节传播常数和波导参数的方法,可以得到非局域、振荡、局域三种类型的表面波. 波导参数和传播常数之差大于阈值时,线性电介质和中心对称光折变晶体界面可以形成局域表面波. 波导参数为正值时,局域表面波主要聚集在中心对称光折变晶体内,随着传播常数的增大,波能量随之单调递增,表面波可以稳定传播. 在给定的条件下,调节决定非线性作用强度的可变参量可以控制局域表面波模的阶数和传播波形. 关键词： 非线性光学 中心对称光折变晶体 表面波     

基于二维特异材料波导的表面电磁波的慢波实验研究

本文在理论分析的基础上,实验研究了二维MNG/DPS/MNG(磁单负材料/双正材料/磁单负材料)表面波波导中的慢波效应.该波导的色散曲线随着电路参数(单元电容)的改变而改变,而且在色散曲线的截止频率点,电磁波的群速度理论上等于零.因此可以通过改变MNG区域的电路参数,得到在不同截止频率的慢波特性.另外,本文还通过改变MNG区域的电路参数实现在某一固定频率下波速度渐变的慢波效应.实验结果与仿真结果相一致.     

聚焦光束在半无限大生物组织内传播的Monte Carlo模拟

分析了聚焦光束在介质中的传播情况,利用VC++语言编制了一套平圆光束聚焦在半无限大生物组织内传播的Monte Carlo模拟程序,对几种不同参数值的情况进行了模拟,通过对模拟结果的分析,得出了平圆光束聚焦在半无限大生物组织内传播的规律。     

Coherent transmission and reflection spectra of ordered structures from spherical alumina particles

In this paper, two novel types of semi-slow light photonic crystal waveguide with large transmission bandwidth obtained by shifting the boundaries of a W1 waveguide in the direction of light propagation are presented. One includes air rings localized at only one side of the line defect and the other replaces the holes at each side of the waveguide by the uniform air rings which are constructed by the homocentric square dielectric rod inserted into the air holes. The structure produces unusual “n-type” transmission spectrum depending on the different parameters such as inner radius of air ring, dielectric constant of square dielectric rod, etc. It is shown that the transmission spectra of the two structures are completely different from each other. A versatile control of light propagation with large normalized bandwidth and slow light phenomena can be obtained using a unique geometrical parameter. Numerical simulation by the finite-difference time-domain (FDTD) method demonstrates the propagation of the broadband pulse.     

Investigation of THz Sommerfeld wave propagation on single-wire at different temperature

In this paper, THz Sommerfeld wave propagation on dielectrically coated cylindrical metal wire and conical metal wire is presented. The propagation characteristics of single wire are largely related to the characteristics of material being used, which may change significantly with the temperature variation. Then, the surface wave propagation along the THz wire waveguide is investigated by the numerical calculation from 0.1 to 1 THz at different temperature. The influences of different conductivity and different temperature on the propagation characteristics of the dielectrically coated cylindrical metal wire and conical metal wire are discussed, including electric field distribution, propagation loss and energy coupling characteristic. The analysis results release a fundamental characteristic for describing the THz surface wave propagation on single wire at different temperature, and moreover, the analysis results also suggest that the single wire is a promising THz waveguide and very useful for the space sensing at cryogenic temperature in future.     

基于Warping变换的波导时频分析

海洋波导的存在使得信号在水中传播过程中产生频散, 从而降低了信号处理质量. 基于声场的波导不变特性, 给出了一种具有普遍意义的Warping变换, 这种变换可以将波导中的信号频散特性简单化. 数值仿真结果表明, 只需要知道波导不变量的取值范围就可以很好地提取出波导的频散曲线, 数值仿真和海上实验数据给出了较为理想的结果.     

Gap solitons in defocusing lithium niobate binary waveguide arrays fabricated by proton implantation and selective light illumination

Photovoltaic photorefractive binary waveguide arrays are fabricated by proton implantation and selective light illumination on top of an iron-doped near stoichiometric lithium niobate crystal. Linear discrete diffraction and nonlinear formation of gap solitons were investigated by single-channel excitation using Gaussian light beams coupled into either wide or narrow waveguide channels. The results show that, at low power, linear light propagation leads to discrete diffraction, whilst for higher input power the focusing mechanism dominates, finally leading to the formation of gap solitons in the binary waveguide arrays. Our simulation of light propagation based on a nonlinear beam propagation method confirms the experimental findings.     

Guided waves in anisotropic media

This paper investigates the propagation of electromagnetic waves in a dielectric anisotropic medium containing conducting planes. A plane and rectangular waveguide is considered for certain particular cases of the orientation of the principal axis of the anisotropic medium relative to the waveguide coordinates. The dispersion equations for the propagation constants are deduced.In conclusion we thank D. A. Dobrotin for his advice.     

阵列波导光栅解复用器的标量传输理论及其简化模型

以波导本征模式场作输入光场,阐述了AWG中实际光场的传输数学模型,对输入场作高斯近似,阐述了光场传输的简化模型.通过简化模型与实际情况的比较,肯定了高斯近似简化模型在一定情况下的合理性.对于给定串扰要求,利用高斯近似模型可以决定最外层阵列波导坐标与衍射场光束束腰的比值,对实际器件设计来说有一定意义,但高斯简化模型在一定情况会引入较大误差,精确定量模拟AWG应采用实际光场标量传输模型.     

Sound propagation in two-dimensional waveguide with circular wavefront

Sound propagation through a waveguide is generally modeled by the Webster horn equation which assumes a planar pressure wavefront. However, most of the sources are non-planar in nature. In this work, a 1-D model is derived for sound propagation through a 2-D waveguide with circular wavefront. The model is derived from the 2-D Helmholtz equation using the weighted residual method. The model assumes a uniform pressure across the angular coordinate at a given radial distance. A 2-D finite element model is used to validate the results for different waveguide geometries and it shows good agreement.     

Analysis of Planar Dielectric Waveguide with Mirror-Conjugate Chiralities in the Core and the Cladding

The propagation characteristics of a planar waveguide with mirror-conjugate chiralities filled in the core and the cladding (mirror-conjugate chirality waveguide) are presented. The effects of chirality on cutoff, dispersion and field distribution characteristics of the waveguide are studied. The results show that the waveguide with desired features can be made by appropriately selecting the chiralities of the core and the cladding, because the core chirality and cladding chirality have different influences on waveguide propagation characteristics.