基于三角谐振环的新型六边形谐振环金属线复合周期结构左手材料性质研究

通过实验及仿真研究了三角谐振环组合新型六边形谐振环金属线复合周期结构左手材料.仿真研究了以金属铜三角开口谐振环（SRRs）为基本单元的周期结构负磁导率材料,与闭口环（CSRRs）结果对比发现三角开口谐振环能产生很好的谐振效果即能产生负磁导率,并且多层单元仿真发现多个谐振环耦合能提高谐振频率并加宽谐振频段;设计、制作并实验和仿真研究了三角开口环为基本单元的六边形谐振环金属线复合周期结构左手材料,仿真结果在98GHz附近出现良好负折射效应,实验验证在93—108 GHz出现良好负折射效应,与仿真结果具有良好的一致性.该研究对新型周期结构左手材料的研究、设计和研制具有重要的科学意义和应用前景. 关键词： 左手材料 三角环组成的六边形谐振环 负折射     

一种新颖的变异开口谐振环双频带磁谐振特异材料

根据磁谐振等效电路原理,设计出了工作在X波段的基于变异开口谐振环(split ring resonators)结构的新型双频带磁谐振特异材料.由于内外环间具有弱耦合的优越特性,所提出的磁谐振特异材料的两个工作频点可以较为方便地调节.该研究成果为特异材料的多频带、宽带化提供有益的的研究思路和设计方法. 关键词： 磁谐振特异材料 双频带 弱耦合     

非对称开口六边形谐振单环的微波透射特性

受自然界树型结构的启发，设计了分叉树型微结构单元，用电路板刻蚀技术制作了非对称开口六边形谐振单环及其组合结构.采用计算机模拟和实验研究了单个和多个谐振环在微波段(7—12 GHz)的电磁响应行为.研究结果表明：该结构具有负磁导率特性，开口谐振环几何尺寸影响环的磁谐振频率；两环环间距较小时出现二次谐振；带高级分支的辐射状环列相对于不带分支环列透射峰向低频移动.实验和模拟结果相符. 关键词： 负磁导率 开口谐振环 透射率     

基于斜三角开口对环的宽带低耗左手材料

本文将磁谐振环-金属线共面结构与磁谐振环相结合, 提出了一种基于斜三角开口对环结构的新型宽频带低耗左手材料结构. 该结构能产生两个磁谐振, 实现两个双负频段. 研究表明, 调节单元尺寸可使两个双负频段移动重合形成一个宽频带. 理论分析、仿真和测试结果均表明, 本文提出的新形结构在9.3—13.2 GHz频段同时具有负的磁导率和负的介电常数, 相对带宽34.7%, 损耗性能系数347.9, 实现了宽带低耗左手材料. 其研究结果对多频段、宽带低耗左手材料的设计具有重要的指导意义.     

基于开口环的可调谐滤波器及其电磁带隙

基于开口谐振环上加载变容二极管设计可调谐滤波器,很好地实现了电磁波带隙的可调.在单环开口谐振环缝隙处或者双环开口谐振环的两环之间加载变容二极管,改变加载变容管上得的电压,改变该结构的分布参量而达到滤波器可调性能.同时通过数值计算分析了该滤波器结构对电磁波的频率响应函数,指出其形成电磁波带隙的物理机制,为了消除开口谐振环的磁谐振效应而关闭开口谐振环的缝隙实验进行了验证.研究表明基于变容管开口环的可调谐滤波器所形成的电磁波带隙中,有的带隙是源于磁谐振机制.有的带隙是源于电谐振机制.对该滤波器形成带隙物理机制的研究,可以更好地理解开口谐振环,有助于其在光学和微波波段器件的设计.     

基于矩形谐振环的新型复合周期结构左手材料研究

通过实验及仿真研究了基于矩形谐振环的新型三角形和三矩形开口谐振环金属线复合周期结构左手材料.仿真研究了以金属铜三角谐振环和三矩形谐振环（SRRs）为基本单元的周期结构负磁导率材料,结果显示两种谐振环均能产生很好的谐振效果,即能产生负磁导率;设计、制作并实验和仿真研究了三角谐振环和三矩形谐振环金属线复合周期结构左手材料,实验结果分别在9.5—13.3GHz和9.8—12.5GHz出现良好的负折射效应,与仿真结果具有较好的一致性.该研究对新型周期结构左手材料的研究、设计和研制具有重要的科学意义和应用前景. 关键词： 左手材料 负折射 三角形谐振环 三矩形谐振环     

基于发卡式开口谐振环的柔性双频带超材料

本文设计了一种基于开口谐振环(split ring resonator, SRR)混合排列单元格的小型化双频带超材料(metamaterial, MM). 该MM的单元结构为发卡式SRR, 所设计的双频带MM可以应用于无线局域网(2.4 GHz) 和全球微波互联接入(3.5GHz)系统. 并且, 采用柔性介质作为基板增加了MM的柔韧度和普适性, 实验和测试结果表明: 双频带MM的中心频率可以通过调节SRR的尺寸进行控制. 此外, 本文也对MM在不同入射角的情况进行了分析, 结果表明MM对入射角度不敏感.最后, 通过MM的表面电流分布情况研究, 进一步解释了其双频带谐振频率的产生原理.     

一维负磁导率材料中的缺陷效应

理论和实验已经表明，金属开口谐振环（split ring resonators,简称SRR）可以实现材料的有效磁导率μeff在某一频率范围内为负.采用波导法实验研究了不同几何尺寸的六边形SRR在X波段微波作用下的近邻相互作用.实验发现，相同尺寸的六边形SRR周期性排列而成的一维负磁导率材料存在一个谐振频率；当缺陷谐振环引入一维负磁导率材料时，主谐振频率和缺陷环谐振频率同时发生移动；主谐振频率和缺陷环谐振频率的移动量随缺陷与双环谐振频率之差的增加而减小，当缺陷环谐振频率与双环谐振频率接近时，环间的相互作用增强，频率的移动量增大. 关键词： 负磁导率 缺陷效应 开口谐振环     

二维负磁导率材料中的缺陷效应

研究了以金属铜六边形开口谐振环为基元的二维负磁导率材料的缺陷效应.利用电路板刻蚀 技术制备了二维负磁导率材料样品.采用波导法测量了点缺陷和线缺陷对二维负磁导率材料X 波段(8—12GHz)微波透射行为的影响.实验发现，无缺陷的二维负磁导率材料样品存在一个 谐振频率，在稍大于该谐振频率的极窄区域内表现为负磁导率.点缺陷和线缺陷SRR的引入导 致材料主谐振峰的强度下降、谐振频率发生移动，品质因数Q显著下降.缺陷的存在破坏 了材料的周期性结构，从而引起其谐振峰的谐振强度和谐振频率发生变化.缺陷效应的研究 不 关键词： 负磁导率 缺陷效应 开口谐振环     

超材料谐振子间的电耦合谐振理论与实验研究

通过将两个金属开口环谐振器口对口地放置, 实现了超材料谐振子间的电耦合谐振. 对电耦合谐振的微波等效电路进行了理论分析和数值计算, 结果表明耦合后的超材料谐振子能产生两个谐振频率, 其中一个随耦合强度的增加逐渐向低频方向移动, 而另一个固定在单谐振子的谐振频率处不变. 微波透射谱的实验测试和电磁仿真结果表明, 两个谐振峰随耦合强度的增加分别向低频和高频方向移动. 分析表明: 低频谐振峰的位置主要是由超材料谐振子间的电耦合强度决定的; 高频谐振偏离单谐振子的谐振频率主要是由不可避免的磁耦合引起的, 而且在耦合间距越小时磁耦合影响越大. 提出的基于超材料谐振子间的电磁耦合实现的双频谐振及其可调性极大地增加了超材料的设计与应用空间.     

同时实现介电常数和磁导率为负的H型结构单元左手材料

基于用一种结构同时实现材料介电常数和磁导率为负的思想，提出了H型结构单元左手材料模型.采用矩形波导法测试表明，H型结构单元在微波频率范围出现左手透射峰，并且可以由参数t对左手特性区域进行调控.同时利用相位法、棱镜折射法和散射参量法从实验和理论证明了在左手透射峰区域材料的折射率为负值，介电常数和磁导率亦同时为负.相对由金属开口谐振环与金属线两种结构组合实现的左手材料，H型结构集磁谐振与电谐振于一体，结构简单、制备方便，对微波器件左手材料表现出更多的优越性.     

Microwave and MM-wave magnetoelectric interactions in ferrite-ferroelectric bilayers

Measurements of the strength of magnetoelectric (ME) interactions at microwave and millimeter-wave frequencies have been carried out on layered ferrite-piezoelectric oxides. An electric field E applied to the composite produces a mechanical deformation, resulting in a field shift δH_E or a frequency shift δf_E in the resonance. A stripline structure or a cavity resonator was used. The strength of ME coupling is obtained from data on δH_E or δf_E vs. E. Studies were performed at 1–110 GHz on bilayers of single crystal nickel zinc ferrite or hexagonal ferrites and single crystal lead magnesium niobate-lead titanate, lead zinc niobate-lead titanate or polycrystalline lead zirconium titanate. The coupling strength has been found to be dependent on the nature of piezoelectric phase, magnetic field orientation and volume for both phases. The ME coupling strength is on the order of 1–2 Oe cm/kV (or 3–6 MHz cm/kV) and is an order of magnitude stronger than in polycrystalline ferrite-piezoelectric bilayers. The high frequency ME effect is of importance for dual electric and magnetic field tunable ferrite-piezoelectric devices.     

Reconfigurable subwavelength waveguide based on magnetic metamaterial

The design and characterization is described of a reconfigurable subwavelength waveguide based on magnetic metamaterial. The waveguide is capable of reconfiguring its propagating mode from right-handed to left-handed, which can be applied in the design of novel microwave and RF devices such as leaky wave antennas with broadened scanning range. The waveguide consists of a rectangular metallic waveguide loaded by two pieces of different magnetic metamaterials, which are structured by the same cells—modified split ring resonators (MSRRs)—with different arrangements. Positions of the two pieces of metamaterials in the waveguide can be reconfigured separately by the control mechanism. The simulated transmission data show that the waveguide has a passband below the cutoff frequency of the hollow waveguide either in the left-handed case or in the right-handed case. The extracted constitutive parameters have demonstrated that the effective permittivity and permeability of the waveguide are simultaneously negative in the left-handed case and positive in the right-handed case. The magnetic field and surface current distributions in the waveguide confirm that the waveguide operates as can be expected. The influence of the control mechanism on the performance of the waveguide is studied. It is shown that the influence is so minor that it can be neglected.     

基于金属结构单元间耦合的左手材料的设计及实验验证

提出了基于金属结构单元间耦合进行左手材料设计的思想,并建立了理论分析模型.通过合理选择结构单元的结构参数并通过单元之间的耦合,使电谐振等效电路的谐振频率与磁谐振等效电路的谐振频率相等,从而最大限度地实现宽左手频带.加工、制作并测试了基于金属结构单元间耦合的左手材料.实验结果表明,测试样品具有相等的电谐振频率和磁谐振频率,其左手频带的带宽为24 GHz.实验结果与理论分析一致,验证了基于金属结构单元间耦合的左手材料设计思想. 关键词： 左手材料 单元间耦合 等谐振频率 宽频带     

基于双十字架型宽带低耗小单元左手材料的设计与实验验证

提出了一种利用电谐振器与磁谐振器集成于一体的单面左手介质结构设计方案, 该方案采用两个十字架型金属结构镜像并列放置在介质基板的同一侧形成一个左手单元, 并将其排列成周期结构. 软件仿真和优化提取了一系列有效电磁参数, 结果表明, 该结构在9.4–16 GHz的频率范围内等效介电常数和等效磁导率同时为负, 其相对带宽达到了52%, 并且单元电长度和损耗都小于同类型的结构. 对该结构进行了加工、制作并通过波导法测试再次证明了其优良左手特性的存在性. 为左手材料的广泛应用打下了基础.     

Dual bands of negative refractive indexes in the planar left-handed metamaterials

A kind of planar left-handed metamaterial (LHM) with unique configurations is demonstrated, which offers an approach in building dual-band negative-index materials. Simulated and experimental results predict two left-handed transmission bands near 11.1 and 14.6 GHz. Dual bands of negative refractive indexes are verified using the retrieval procedure. Field and current distribution at the dual magnetic resonance are also examined. The effective electromagnetic parameters show that by carefully adjusting dimensions of the unit cell, electric and magnetic resonances can be coexistent at some frequency ranges with both negative permittivity and negative permeability. The idea can help us designing planar negative-index materials with multibands.     

Tunable dual-band ferrite-based metamaterials with dual negative refractions

We report on three types of tunable dual-band metamaterial with dual negative refraction in this paper. The three types of metamaterial are composed of ferrite slabs and three different metallic resonators, including split-ring resonators (SRR), Ω-like resonators, and short wire pairs. The ferrite slabs under an applied magnetic bias provide one magnetic resonance frequency band and the three metallic resonators provide another magnetic resonance frequency band, respectively. The continuous wires within the metamaterials provide the negative permittivity in a wide frequency band covering the two magnetic resonance bands. We give the design, analysis and numerical demonstrations of three such types of metamaterial in detail. The effective electromagnetic parameters obtained from the simulated S-parameters indicate that the three types of metamaterial indeed exhibit two negative refraction passbands and the two passbands can also be shifted by changing the magnetic bias. Our results open the way to fabricate tunable dual-band metamaterial cloaks, absorbers, and antennas.     

一种结构简单的二维左手材料设计及仿真研究

基于产生负介电常数的周期性金属线单元结构,讨论了金属线长度和宽度的变化对负介电常数的影响.在入射波的波矢k方向上放置两个单元结构,使两单元中的金属线响应入射波的磁场产生负磁导率,就可得到一维左手材料.若保持电边界条件的位置不变而调换波端口和磁边界条件位置,即入射波的波矢k转过90°角,两单元结构同样具有左手特性,从而可实现二维左手材料.     

Enhancement of magnetic field intensity with a left-handed metamaterial tunnel resonator for obstacle sensing

A narrow metal strip inspired by the left-handed metamaterial and sensitive LC resonator structure has been released in this work where the narrow metal strip is presented as a tunnel structure which can enhance electric and magnetic properties. A commercially available electromagnetic simulator CST Microwave Studio is utilized to design and investigate the eSRR (electric split-ring resonator) and tunnelled LC resonator structures. Furthermore, ADS (Advance Design software) is used to determine the scattering parameters of the equivalent circuit. The proposed metamaterial structure is employed as a sensor operating in the C-band (6.88 GHz) of the microwave region, and its sensing properties are tested using glossy paper as an obstacle. The designed metamaterial tunnelling structure exhibits very high sensitivity toward dielectric obstacles at different rotational angles and thus can be potentially used in various sensing applications. The field enhancement effects on sensing application are verified by measured obtained results for eSRR and tunnelled LC resonator structures.     

A compact square-shaped left-handed passive metamaterial with optimized quintuple resonance frequencies for satellite applications

The research aims to develop a more sophisticated novel left-handed and compact square-shaped metamaterial (SM) inspired multi-frequency bands like C-, X- and Ku-band applications. Even though the performance of existing satellite application devices are adequate, significant changes in technology over the past decades require advanced and more accurate techniques or devices. Hence, we approach the problem with a broader perspective by integrating a metamaterial structure in satellite application devices. As a general rule, the unconventional material known as metamaterial has extraordinary electromagnetic properties which are impracticable in commercially available materials. It represents an important study topic because this type of peculiar material is generally used in many field applications which encouraged us to experiment with the stated frequency bands by introducing a novel SM design. The novel SM design structure involved a 1.6 mm Epoxy Resin Fibre (FR-4) substrate material. This compact metamaterial design contains nine square rings with an altered small square ring joined in it. The numerical simulation of the SM design for satellite frequencies was performed using the Computer Simulation Technology (CST) Microwave Studio. The scattering parameters of the suggested SM design were determined by utilising Finite Integration Technique (FIT) in CST software. Several parametric studies that were analysed in this study include various design structure, types of substrate materials and SM array arrangement. Based on the adapted simulated frequency range (4 to 18 GHz), the unit cell SM exhibited five resonance frequencies at 5.49 and 7.33 GHz (in C-Band), 9.05 and 11.38 GHz (in X-Band) and 13.48 GHz (in Ku-Band). The measured resonance frequencies of the unit cell were 5.62 and 7.39 GHz (in C-Band), 9.15 and 11.32 GHz (in X-Band) and 13.51 GHz (in Ku-Band). The resonance frequencies obtained from both methods were similar. According to all three resonance frequencies, the SM design manifested a left-handed characteristic. Hence, on this basis, the proposed SM design with unique characteristics is deemed suitable for C-, X- and Ku-bands applications.