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 共查询到19条相似文献,搜索用时 328 毫秒
1.
孙旭  赵青  李宏福 《物理学报》2008,57(4):2130-2135
基于耦合波理论,对两类半径渐变圆波导TE0n-TE0(n+1)模式转换器进行理论分析、数值计算和仿真模拟.均匀半径渐变波导高功率模式转换器,采用中心频率为17.14GHz、六周期TE02-TE03模式和中心频率为34.30GHz、六周期TE01-TE02模式两种设计参数.非均匀半径渐变波导高功率模式转换器,采用中心频率为34.30GHz、六周期TE 关键词: 模式转换器 耦合波理论 非均匀半径渐变 转换带宽  相似文献   

2.
含单负材料的不对称平板波导的传导模   总被引:2,自引:0,他引:2  
陈宪锋  蒋美萍  沈小明  金铱 《光学学报》2008,28(10):1888-1892
利用图解法系统地研究了由不同类型的单负材料作为包层的三层平板波导的模式特征.研究表明单负介质波导具有一系列奇异的特性,与传统介质波导或左手介质波导相比,此波导的芯区横向振荡导模的模折射率范围较大.除0阶导模外,其它TE,TM导模均为芯区横向振荡模,且同阶的TE、TM模的色散曲线几乎重合,只有0阶的TE,TM模才可以支持表面波的传播.单负介质的结构参数对0阶导模的影响较大.一定条件下,波导中可以出现0阶导模的完伞缺失或仅支持表面波的传输,还会出现超慢波现象,甚至可以共生都是后向波的0阶双模.  相似文献   

3.
张强  袁成卫  陈俊  余龙舟  赵雪龙 《强激光与粒子束》2018,30(6):063003-1-063003-4
对比分析了几种可输出圆波导TE01模激励器的仿真设计结果。结果表明,利用行波功分结构实现矩形波导TE10模到4路矩形波导TE10模的等幅同相功分,进而合成转换成圆波导TE01模的转换过程,可在较宽的频带范围内,实现圆波导TE01模的高效激励。以中心频率9.40 GHz仿真设计的圆波导TE01模激励器,在中心频率上的传输效率超过99.9%;在9.08~9.61 GHz的频率范围内,传输效率大于99%。实验测量结果表明,所加工激励器在较宽的频带范围内,传输损耗优于-0.2 dB,与仿真结果的差异主要来自于波导壁面的欧姆损耗和波同转换结构;器件工作频带内平坦特性良好,有利于开展测量工作。  相似文献   

4.
含左手材料对称三层平板空气波导的模式特性   总被引:3,自引:1,他引:2  
研究了左手材料作为衬底及覆盖层的对称三层平板空气波导的传输特性.快波和慢波都可以在这种波导中传播.快波不存在基模模式,只有0阶和1阶的TE或TM模才会出现慢波.当左手材料的相对介电常量和相对磁导率相等时,TE、TM模式完全简并,当其相异时简并消除.可以存在同阶模式的双传播模.  相似文献   

5.
王五松  张利伟  张冶文  方恺 《物理学报》2013,62(2):24203-024203
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.  相似文献   

6.
王强  周海京  杨春  李彪  何晓阳 《物理学报》2013,62(11):115204-115204
从模式保留和转换的角度, 过模波导器件可分为模式转换器、模式保留器和模式综合器. 传统方法只解决其中一种器件的设计或者对器件的某个指标进行改进. 本文在深入分析耦合波理论之后, 提出了过模波导器件的迭代设计方法, 从原理上解决了过模波导器件的设计问题. 该方法能够统一设计三类过模波导器件, 通过添加不同的结构控制方法, 可得到转换效率更高、带宽更宽、结构更紧凑、满足不同工程需求的器件, 而且还能有效设计一些新型器件. 给出了两个设计实例: 双频TM01–TE11模式变换器和光壁馈源喇叭. 双频TM01–TE11模式变换器的两个工作频点为8.75 GHz和10.3 GHz, 波导半径为16 mm, 在两个频点转换效率为99%以上. 光壁馈源喇叭实现TE11模式向高斯束的转换. CST仿真结果验证了这两个器件设计的正确性和有效性. 关键词: 耦合波理论 模式转换器 模式过渡器 迭代法  相似文献   

7.
王奇  薛秉章  蔡英时 《物理学报》1988,37(5):760-768
本文研究了特定边界条件下非对称型Kerr类介质膜漏波导中TE0光波的传播特性。计算结果表明,介质膜厚存在一临界值。临界值之上没有导波存在,临界值之下能同时存在强场TE0模和弱场TE0模,它们具有不同的传播波数。这两个模的膜内传播功率、场强峰值位置随膜厚和光场频率的变化各不相同,色散关系也有极大差别。在对称极限之下,弱场TE0模的色散为零。 关键词:  相似文献   

8.
加载异向介质非辐射介质波导中的慢波传输及应用   总被引:3,自引:0,他引:3       下载免费PDF全文
杨锐  谢拥军  王元源  傅焕展 《物理学报》2008,57(9):5513-5518
将开口谐振环作为加载单元,分析了含有开口谐振环结构非辐射介质波导的新型传输特性.由于异向介质的双各向异性效应,纵剖面磁波型和纵剖面电波型在此新型非辐射介质波导中的传输速度能够减慢,甚至达到零速度.对于波导中的能量关系也进行了分析,研究表明,在一定情况下,慢波传输将引起功率流动的增强.这些特性使得此新型非辐射介质波导更能满足小型化的设计要求. 关键词: 开口谐振环 异向介质 非辐射介质波导 慢波传输  相似文献   

9.
王茹  王向贤  杨华  叶松 《物理学报》2016,65(9):94206-094206
通过棱镜耦合激发非对称金属包覆介质波导结构中的TE0导波模式, 利用两束TE0模的干涉从理论上实现了周期可调的亚波长光栅刻写. 分析了TE0模式的色散关系, 刻写亚波长光栅的周期与激发光源、棱镜折射率、光刻胶薄膜厚度及折射率之间的关系. 用有限元方法数值模拟了金属薄膜、光刻胶薄膜和空气多层结构中TE0导模的干涉场分布. 研究发现, 激发光源波长越短, TE0 模干涉刻写的亚波长光栅周期越小; 光刻胶越厚, 刻写的亚波长光栅周期越小; 高折射率光刻胶有利于更小周期亚波长光栅的刻写. 相较于表面等离子体干涉光刻, 基于TE0 模的干涉可在厚光刻胶条件下通过改变激发光源、棱镜折射率、光刻胶材料折射率、特别是光刻胶薄膜的厚度等多种方式实现对亚波长光栅周期的有效调控.  相似文献   

10.
沈文渊  王虎  耿志辉  杜朝海  刘濮鲲 《物理学报》2013,62(23):238403-238403
基于不规则波导模式匹配法以及缓变波导中电磁波模式耦合理论,研究了一种W波段圆波导TE62模式激励器. 该波导模式激励器采用矩形波导TE10模式通过侧壁耦合馈入同轴波导,利用同轴波导的选模特性激励TE61模式;随后利用轴向半径周期微扰的圆波导实现TE61–TE62模式变换. 文中推导了矩形-同轴波导模式匹配理论,系统研究了波导结构缓变参数对模式变换效率的影响,完成了模式变换器的优化仿真设计,数值计算结果表明:中心频率处TE62模式的转换效率为94.5%,纯度为98.16%,效率85%以上带宽达到1 GHz,能够满足回旋管冷测的要求. 关键词: 同轴波导 模式变换 耦合模理论 半径微扰  相似文献   

11.
We study guided modes propagating along a dielectric slab waveguide with a left handed material (LHM) cover or substrate. The dispersion relation is derived by using normalized waveguide parameters. An analytical method is then proposed to calculate the universal dispersion curves. Different from a slab waveguide with a LHM core, we find that guidance properties are strongly dependent on dielectric permittivity ε and magnetic permeability μ of the substrate and cover layers. For oscillating guided modes, fundamental zero order mode is not always absence, sometimes it exists in a restricted range of normalized propagation constant. First order mode behaves as other higher order modes and exists up to infinite high frequency. Higher order modes have no double degeneracy in the case of LHM cover layer. For surface guided modes, the existence and the type of the mode solutions with respect to different parameters are classified systematically and discussed in detail. Unlike a slab waveguide with a LHM core where the dispersion curve of TE1 surface mode continues with that of oscillating TE1 mode, the dispersion curve of TE1 surface mode continues with that of oscillating TE0 mode. It seems that the two different kinds of modes compensate each other to form one whole mode. Both TE and TM guided modes are discussed.  相似文献   

12.
电磁波在负折射材料填充的3层平板波导中的传播特性   总被引:1,自引:1,他引:0  
柯尊淦  吴少平  郑丹 《应用光学》2008,29(5):825-829
从电磁场理论出发对负折射材料填充的3层平板波导的传播特性进行研究,并进行了数值计算,分析TE和TM波在平板中传播的性质,得到了电磁波的模式方程,与电磁波在右手材料填充的平板波导中的传播特性做了对比,考察了TE模式的能流密度,进行了归一化计算。结果分析表明:基模、一阶模不存在,且任何模式都存在一个截止厚度,随着厚度的增大,模式数量也增多;在一定的入射频率下,平板薄膜厚度趋向一定数值时,可以同时传播多种模式的波,并且入射波频率越高,波导同时存在多种模式的可能性越大;与右手材料相比,左手材料填充相同尺寸的3层平板波导可以传播更高能量的电磁波,导波效果更好。  相似文献   

13.
If the metal cladding of a dielectric optical waveguide is sufficiently thin to be only partially reflecting, then the waveguide modes differ from those of the conventional metal-clad waveguide. The TE modes are little affected by a variation in the metal thickness but the TM modes change considerably due to a coupling between the waveguide modes and the surface plasma waves supported by both the metal: dielectric interfaces and the metal film. It is the refractive index of the dielectric cladding which is remote from the guiding core that determines whether the lowest order TM mode is the TM0 or TM1 mode. This dielectric cladding also strongly influences the attenuation of the TM modes and, if the guide supports a TM0 mode, then the attenuation of the TM modes far from cut-off are an order of magnitude higher than that of the corresponding modes when the guide cannot support a TM0 mode. If the guide can support a TM0 mode then its dimensions can be chosen such that it will support the TEN and TMN modes with equal phase velocities. A lossless approximation is used to develop an expression which will specify the required guide dimensions directly and parametric plots of these dimensions are discussed.  相似文献   

14.
We present a design of a dual-core leaky waveguide that can be used as an integrated-optic polarizer. The proposed polarizer works on the principle of mode filtering. The structure is characterized by two cores, namely core-1 and core-2 and a high index layer in the upper-most region, such a structure supports leaky modes. The leakage losses of the modes have been calculated by using the transfer matrix method (TMM). Single polarization operation is ensured by high differential leakage loss between fundamental TE and TM modes. We show TE-pass operation with 0.5 dB/mm loss in TE0 mode and 13 dB/mm loss in TM0 mode, and TM-pass operation with 0.36 dB/mm loss in TM0 mode and 7.45 dB/mm loss in TE0 mode. Besides single-polarization operation, single-mode operation of the structure is ensured by high leakage loss of all the other higher-order modes.  相似文献   

15.
We present the general theory of rippled wall mode converters. Coupling coefficients for TE and TM waves, of both fixed and rotating polarizations, are calculated. The waveguide ripples considered may be axisymmetric, fluted or helical. We describe in detail a 97% efficient TE04/TE01 converter designed for use with a 35 GHz gyrotron. Cold test results confirm its performance.  相似文献   

16.
Based on classical electromagnetic theory, characteristics of guided modes in a rectangular waveguide filled with a pair of single-negative layers are studied. The results show that only surface waves of TE mode can propagate in this peculiar waveguide, no TM mode in any forms can propagate in it. In addition, TE waveguide modes will be affected by permeability ratio μ1/μ2 and dielectric layer thickness ratio P. Finally, from the electric field distribution of TE mode, we find the amplitude and location of the electric field can be adjusted by changing the thickness ratio P.  相似文献   

17.
Dispersion equations for TE and TM modes in width-limited waveguides formed by parallel cylindrical surfaces are derived in adiabatic approximation. It is shown that the dominant TE01 mode is strongly localized in the waveguide center.  相似文献   

18.
The conversion of guided modes (TE0 and TE1) at a rectangular step on a dielectric slab waveguide is investigated with mm microwaves. The power of the modes is measured from their interference patterns in the evanescent field outside the waveguide slab. The relative power of two modes changes periodically when the length of the step is varied. In the experiments a change of up to three orders of magnitude was measured. The step is considered as a sequence of three waveguide sections of different thickness. At the discontinuities the modal fields are assumed to illuminate the next section. The calculation based on this model agrees with the experimental results.  相似文献   

19.
The optical characteristics of the asymmetric metal-clad waveguide are analysed, more accurate formulae are derived for calculating the propagation constants and loss coefficients of TE and TM modes. The computed results for Al/GaAs/AlGaAs waveguides are in good agreement with the numerical results, and are much more accurate than the results in some other papers. The method for selecting the TE0 mode is presented and discussed.  相似文献   

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