共查询到20条相似文献,搜索用时 177 毫秒
1.
设计实现了一种基于双圆弧形金属结构的宽带反射型极化旋转超表面, 在7.9–20.1 GHz的宽频带范围内交叉极化转换率达到99%, 通过改变其结构参数可实现在保持高效的交叉极化转换率的条件下对交叉极化反射相位的自由调控. 基于六种不同结构参数极化旋转超表面结构单元的空间排布设计实现了一维宽带相位梯度超表面, 在宽频带内, 实现了异常反射. 测试了其镜面交叉极化反射率, 与仿真结果基本一致. 仿真计算了x-极化波入射时的电磁场分布和异常反射角度, 与理论计算结果基本一致. 仿真与测试结果均表明这种相位梯度超表面在8.9–10 GHz 和10.0–18.1 GHz的两个宽带频率范围内可分别实现高效的表面波耦合和异常反射. 相似文献
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针对圆极化波, 通过同极化反射超表面结构单元的空间排布, 设计实现了一种二维非色散高效相位梯度超表面. 同极化反射相位可以通过同极化反射超表面结构单元金属线的面内旋转来自由调控. 实现的相位梯度超表面可对左右旋入射波产生相反的相位梯度. 当线极化波入射到超表面上时, 反射波被分为两束向相反方向传播的圆极化波. 仿真了线极化波垂直入射时的反射功率密度谱, 仿真结果与理论上设计的异常反射方向一致. 制作了厚度为2 mm的超表面样品, 测试了其镜面反射率曲线. 实验结果表明, 线极化波垂直入射时, 超表面在9.5-19.0 GHz的镜面反射率降至-5 dB以下. 相似文献
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为了获得特定的探测器光谱响应,可以采用全滤色片法对滤色片进行精确匹配.在匹配计算时,通常使用滤色片的垂直光谱透过率作为计算依据;而实际应用中斜入射的光线会导致匹配计算结果和测试结果不一致.本文在光线漫入射条件下对圆柱形状滤色片的漫入射光谱透过率计算方法进行了分析,提出了一种由滤色片垂直入射光谱透过率计算滤色片漫入射光谱透过率的修正模型.设计了双积分球测量装置对滤色片的漫入射透过率进行检测.在该装置下检测不同滤色片的漫入射光谱透过率,并与修正模型计算结果进行对比验证.实验结果表明,修正模型可以在较小误差范围内由滤色片的垂直入射光谱透过率计算其漫入射光谱透过率,应用于全滤色片匹配可以显著提高匹配结果和实际测量结果的一致性. 相似文献
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基于圆极化波入射条件下的高效同极化反射超表面实现了对圆极化反射波相位的自由调控, 设计了一维圆极化波反射聚焦超表面. 在中心频率f=16 GHz附近, 右旋圆极化平面波入射时, 反射波聚焦于焦距L=200 mm的实焦点; 左旋圆极化波入射时, 反射波近似聚焦于焦距L=-200 mm的虚焦点. 仿真计算得到聚焦波束的波束宽度、焦深. 结果表明, 这种圆极化反射聚焦超表面具有很好的聚焦效果, 同时具有长焦深和宽带特性. 相似文献
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角锥棱镜的误差引起的反射光束相位误差分析 总被引:2,自引:0,他引:2
提出一种计算角锥棱镜反射光束相位误差的方法.光束通过非理想角锥棱镜时会引入一个附加光程差,从而改变光束的相位特性和反射光束的传播方向.在小误差近似条件下,采用光线追迹法建立了一个有效的数学模型,计算角锥棱镜的二面角误差和反射面面型误差引起的传输光束的附加相位,并分析了该模型的理论误差.在二面角误差为1",反射面面形光圈数小于0.5的条件下,该模型的数值仿真结果显示角锥附加相位具有高度的中心对称性,附加相位对入射光束引入的相位平均斜率为零,这一特性与误差的种类和大小无关.角锥棱镜的附加相位模型为分析其在应用中给系统带来的误差提供了一个新的方法,有助于指导不同应用场景中所使用角锥棱镜的加工指标要求. 相似文献
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提出了一种测量非透明材料表面光学非线性的新方法:挡板反射4F测量法。该方法在反射4F相位相干成像系统的基础上,在4F系统的像平面放置一个与系统入射面光阑相匹配的不透明挡板,通过测量不同情况下的反射率,实现对材料光学非线性的测量。详细介绍了该方法的基本原理,并通过数值模拟计算了入射角对测量灵敏度的影响。该方法具有单脉冲测量,可同时得到材料的非线性吸收与折射系数等特点。结果表明,在相同条件下挡板反射4F测量法的灵敏度比反射Z扫描方法高2个数量级。 相似文献
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用瑞利-傅里叶(Rayleigh-Fourier)数值方法及椭偏测量,研究了高反射正弦形浅光栅的偏振特性.当正向入射条件下,光栅周期与波长之比满足某一关系时,其反射光电场的两垂直方向分量相移差大的特性,制成了一种新颖的双折射滤光片,文中给出了这种双折射滤光片的初步实验结果. 相似文献
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针对相位梯度超表面在隐身技术中的应用,提出通过表面波耦合和异常反射两种机制复合实现宽频带后向雷达散射截面(RCS)缩减,采用开口谐振环进行相位梯度设计,实现了一种二维极化无关相位梯度超表面,在10 GHz附近,超表面通过将垂直入射电磁波耦合为表面波实现RCS缩减,而在大于11 GHz的频率范围内,相位分布的不均匀性使垂直入射的电磁波发生漫反射或者异常反射,降低后向RCS,制作了厚度为2 mm的超表面样品,测试了其反射率曲线和后向RCS,并与相同尺寸的金属板进行了对比,实验结果表明,在宽频段内(9.5—17.0 GHz),超表面在垂直入射情况下可将后向RCS缩减至少10 dB,由于厚度薄、重量轻、频带宽,RCS缩减超表面在隐身新材料和新技术方面具有很大的应用潜力。 相似文献
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本文从角谱理论出发建立了涡旋光束在空气-玻璃界面反射时的傍轴传输模型, 并研究了反射过程中诱导产生的正交偏振效应. 当一水平偏振涡旋光束以不同角度入射时, 反射光束的正交偏振分量呈现出类似于一阶厄米-高斯模式的双峰强度分布, 而水平偏振分量强度分布呈现与入射光束相似的分布, 且只在布儒斯特角附近入射时才现出与正交偏振分量垂直的双峰分布. 对于任意线偏振入射光, 其正交偏振分量的偏振方向不再垂直于入射时的偏振方向, 而是与反射光束的中心波矢垂直, 此时正交偏振分量出现有趣的旋转特性, 其物理原因归结于任意线偏振光入射时所对应的水平与垂直偏振分量的反射系数不同. 最后进行了相关实验验证, 发现实验结果与理论分析符合得较好.
关键词:
正交偏振
涡旋光束
任意线偏振 相似文献
10.
由于沙地通常处在半干旱地区,在风蚀作用下表面结构特征会有所改变,同时,沙地表面粗糙度与组成成分的时间与空间变化也是研究风蚀模型所必须的输入信息。作为一种非接触的探测手段,遥感技术有助于实现对沙地表面粗糙程度在时空尺度上的研究。为了利用反射特性描述沙地表面结构特征,以人为模拟的粗糙沙地表面为研究对象,基于野外实测多角度高光谱反射信息,分析了沙地表面粗糙度变化对反射信息分布的影响,并且结合双向反射模型,试图利用模型参数反演粗糙度特征。通过研究发现,如果按照入射方向与沙地表面沙垄方向分类来看,与入射方向平行或者垂直均会对沙地表面反射分布特性有所改变。当沙垄方向与入射光方向垂直时,会使后向散射的反射峰值增加;而沙垄方向与入射光平行时,会使后向散射峰值向主平面两侧扩张。双向反射模型可以模拟沙地表面的反射特性,根据模型参数的变化也可以表示出沙地表面的粗糙度变化特性。这表明双向反射信息可以用于量化沙地表面结构特征,而且有助于了解结构特征对沙地光学特性的影响,也为研究颗粒介质固有光学特性以及反演沙地表面结构特征提供依据。 相似文献
11.
《Physics letters. A》2020,384(31):126813
High impedance surface (HIS) is an electromagnetic band gap (EBG) material that shows magnetic conductor surface properties within its band gap frequencies. The operation bandwidth is corresponding to the frequency range, where the reflection phase varies between +90∘ and −90∘. In this paper, a dual-band HIS is investigated based on planar periodic graphene arrays placed on a grounded dielectric substrate. Analytical circuit model of the graphene array together with the transmission line theory is employed to analyze the proposed structure. We demonstrate that the HIS bands can be adjusted by tuning the geometrical parameters of the structure and the Fermi level of graphene. The graphene-based HIS promises future applications in the low-profile, high gain and high efficiency antennas at THz frequencies. 相似文献
12.
Xavier Begaud Fabrice Linot Michel Soiron Christian Renard 《Applied Physics A: Materials Science & Processing》2014,115(2):517-522
This paper presents an analytical model to design a self-complementary connected antenna array above artificial materials like high impedance surfaces (HIS). The objective of this model is to perform parametric studies to facilitate deeper understanding of a complex antenna array with a significantly shorter computation time than with electromagnetic simulators. The model of the complete structure has been designed in receiving mode when structure is illuminated with a plane wave and using transmission line model and ABCD matrix. By applying an interesting property which gives equivalence between the input impedance in transmit mode and the surface impedance in receiving mode, the impedance match of the self-complementary connected antenna array can be quickly calculated. It is also simple to evaluate the influence of the incidence angle on the reflection coefficient of a self-complementary connected antenna array above perfect electric conductor (PEC) or HIS. PEC or artificial materials can modify the antenna array behavior by either increasing the bandwidth or by adding additional bandwidths. All these results have been verified to be accurate by numerical simulations done with Ansys HFSS. 相似文献
13.
为进一步提高传统Salisbury屏的吸波性能, 本文提出了利用高阻抗表面在特定频率同相反射的特性, 替代原有结构中的金属平板设计多频带Salisbury屏的方法. 通过分析不同频率电磁波经高阻抗表面反射后空间电磁场的场强分布, 说明可以通过共用Salisbury屏的损耗层, 在高阻抗表面同相反射的特征频率附近引入新的吸收带. 以不同尺寸方形周期结构的单频和双频高阻抗表面为例, 从仿真和实验两个方面验证了多频带Salisbury屏设计的可行性, 且实验和仿真结果十分符合. 结果表明, 多频带Salisbury屏基本保留了原有的吸波性能, 同时又引入了新的吸收峰, 吸收峰的位置和数量与高阻抗表面同相反射的频带位置和数目有关. 与传统的Salisbury屏相比, 在材料增加厚度不足1 mm 的情况下, 多频带Salisbury屏的设计使反射率小于-10 dB的吸波带宽由8.5 GHz增加到10.1 GHz, 且实现了向长波方向的拓展, 最低频率由7.5 GHz拓展到5.98 GHz. 相似文献
14.
Jun-Hee Lim Tian Liu Sung-Soo Kim 《Applied Physics A: Materials Science & Processing》2014,117(3):1401-1407
The microwave absorption of metamaterials composed of split cut wire (SCW) on grounded dielectric substrate has been investigated on the basis of equivalent transmission line circuit. S-parameters (S 11 and S 21) and input impedance are numerically simulated with variations of the thickness and dielectric loss of the substrate and the geometry of the SCW. Magnetic resonance resulting from antiparallel currents between SCW and ground plane was observed at the frequency of minimum reflection loss. The simulated resonance frequency and reflection loss can be explained well on the basis of the circuit theory of an LC resonator. Analysis of the input impedance of the high impedance surface has shown that perfect absorption can be obtained at the optimized impedance-matching condition, which is dependent on SCW width, thickness and the dielectric loss of the substrate. Better insight into the absorption mechanism of metamaterial absorbers can be attained through the parametric analysis on complex impedance of SCW and its relationship with reflection loss. 相似文献
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A novel 35GHz 3dB power divider using coupled transmission line is presented. Unlike conventional Wilkinson divider circuit, only the 50 transmission lines are used in the design. The impedance matching can be achieved by coupled transmission line even mode characteristic impedance. The predicated and measured performances agree well. 相似文献
17.
We have designed a transmission line model of the microwave coupling mechanism for a microwave pumped CO2 laser. The model is a total loss ridge waveguide transmission line having nonuniform impedance. The laser plasma is modeled as a frequency-dependent lossy dielectric and acts as a distributed resistance in the length of the microwave cavity. The coupling structure of the microwaves is designed not to be resonant at the microwave source frequency of 2.45 GHz at 1 kW and propagating the total microwave field energy to be absorbed without internal reflection. An exact solution to this general transmission line propagation constant for a shunt resistance along length of the guide is found. The measurements and predictions of the parameters of the plasma conductivity as a function of the attenuation constant agree closely. 相似文献
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We propose a closed form formulation for the impedance of the metal-insulator-metal (MIM) plasmonic transmission lines by solving the Maxwell's equations. We provide approximations for thin and thick insulator layers sandwiched between metallic layers. In the case of very thin dielectric layer, the surface waves on both interfaces are strongly coupled resulting in an almost linear dependence of the impedance of the plasmonic transmission line on the thickness of the insulator layer. On the other hand, for very thick insulator layer, the impedance does not vary with the insulator layer thickness due to the weak-coupling/decoupling of the surface waves on each metal-insulator interface. We demonstrate the effectiveness of our proposed formulation using two test scenarios, namely, almost zero reflection in T-junction and reflection from line discontinuity in the design of Bragg reflectors, where we compare our formulation against previously published results. 相似文献