共查询到18条相似文献,搜索用时 133 毫秒
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仿真和实验验证了厚度极薄的平面结构超材料吸波体, 该吸波体采用加载交指电容的耶路撒冷十字结构, 通过增加单元间的耦合电容显著降低了其工作频率. 测试结果表明, 该超材料吸波体在1.58 GHz, 吸收率峰值为88.48%, 其厚度为2 mm, 约为1/95工作波长, 吸波体的单元尺寸为11 mm, 约为1/17工作波长. 此外, 通过金属通孔将耶路撒冷十字结构与金属底板相连接, 使其对斜入射横电和横磁极化电磁波具有宽角度吸收特性, 在60°时依然具有较高的吸收率, 且吸收峰频率几乎不发生偏移, 从而使其更具实用价值.
关键词:
极薄
宽角度
超材料吸波体 相似文献
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基于手性结构设计了一种极化不敏感和双面吸波的超材料吸波体.该吸波体的结构单元由手性结构和介质基板组成.仿真的电磁波正、反向入射时超材料吸波体的吸收率表明:该吸波结构的正、反面是互易的,具有双面吸波特性.仿真的不同极化角下超材料吸波体的吸收率表明:该超材料吸波体具有极化不敏感特性.仿真的不同入射角下超材料吸波体的吸收率表明:该超材料吸波体的入射角较窄.仿真的吸波体单元的表面电流和磁能密度分布表明:电、磁场之间存在交叉耦合,吸波与手性有关.仿真的不同损耗情况下超材料吸波体的吸收率表明:基板的介质损耗在吸波过程中起主导作用,金属的电阻热可以忽略不计.该超材料吸波体可能在要求双面吸波的领域中具有潜在的应用.
关键词:
极化不敏感
双面吸波
手性结构
超材料吸波体 相似文献
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目前,很少有文章就如何实现宽角度吸波材料进行详细的理论分析和设计指导,设计宽角度吸波材料仍然是一件很困难的事情.本文基于等效介质理论对带有反射地板的单层介质超材料吸波体进行较为详细的理论分析.从基础电磁理论出发,推导TE波(横电波,电场方向与入射面垂直的平面电磁波)和TM波(横磁波,磁场方向与入射面垂直的平面电磁波)照射下吸波体的反射系数,分析实现宽角度吸波效果所需的等效电磁参数,为宽角度超材料吸波体的设计提供了理论基础.此外,论文还理论分析了实现宽带宽角吸波等效电磁参数所要满足的条件,并做了计算检验.结果表明,当介质等效电磁参数按照特殊曲线随频率发生变化时,理论上能实现宽带宽角的吸波效果. 相似文献
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本文设计了一种超薄螺旋结构超材料吸波体,其厚度(1.034 mm)约为其工作波长(4.81 GHz,6.59 GHz,9.16 GHz,12.69 GHz和13.71 GHz)的(1/60,1/44,1/32,1/23,1/21).仿真和实验结果表明,该吸波体在4.81 GHz,6.59 GHz,9.16 GHz,12.69 GHz和13.71 GHz处吸收率分别达到94.55%、99.89%、99.73%、99.26%和99.41%,实现了多频带强吸收.从表面电流和功率损耗密度两个方面分析了产生强吸收的原因,理论分析表明,多频带强吸收能在五个相邻频率处产生多阶局域表面等离激元谐振,螺旋结构之间强烈的电谐振使超材料结构单元产生强烈的吸收.该超材料吸波体设计简单、易于制作和应用,在电磁波吸收中具有应用价值. 相似文献
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基于电阻膜设计了一种宽频带、极化不敏感和宽入射角的超材料吸波体.该吸波体的结构单元由六边形环状电阻膜结构、介质基板和金属背板组成.仿真得到的反射率和吸收率表明,该吸波体在7.0-27.5 GHz之间对入射电磁波具有宽频带的强吸收,证实了电路谐振相对于电磁谐振易于实现宽带吸波.仿真得到的不同极化角和不同入射角下超材料吸波体的吸收率表明,该吸波体具有极化不敏感和宽入射角特性.仿真得到的基板和电阻膜对超材料吸波体吸收率的影响表明,电阻膜结构和金属背板之间形成的电容以及电阻膜结构的电阻都存在一个最佳值,此时电路谐
关键词:
电阻膜
电路谐振
宽频带
超材料吸波体 相似文献
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设计了一种基于一阶Minkowski分形双方环(Minkowski fractal double square loop, MFDSL)电谐振器结构与电阻膜复合的超薄、 宽频带、极化不敏感和宽入射角的超材料吸波体. 该吸波体的基本结构单元由MFDSL电谐振器结构、方块电阻膜、电介质基板和金属背板组成. 采用时域有限差分算法对这种复合结构吸波体的电磁波吸收特性进行数值模拟分析. 模拟得到的反射率和吸收率表明: 该吸波体在7.5-42 GHz之间对入射电磁波具有大于90%以上的强吸收特性. 模拟得到的不同极化角和不同入射角下的吸收率表明: 该吸波体具有极化不敏感和宽入射角特性. 进一步的数值模拟结果表明, 该复合结构吸波体对电磁波的吸收主要是基于电磁谐振和电路谐振机制, 通过方块电阻的设计可以实现工作频率范围的调节.
关键词:
电阻膜
分形频率选择表面
宽频带吸收 相似文献
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设计了一种三层宽频吸波超材料,其表层和中间层为单元尺寸不同的周期阵列结构,底层为吸波平板结构,优化后的总厚度仅为4.7 mm,并采用三维(3D)打印技术成功制备了该吸波超材料.吸波体反射率测试结果表明,在电磁波垂直入射条件下,宽频吸收峰分别出现在5.3和14.1 GHz,两峰叠加使得其在4-18 GHz频率范围内反射损耗均小于-10 dB.采用S参数反演法计算了每一层的等效电磁参数,并利用多层结构反射率公式推导得出该模型的理论反射率,理论计算结果与实测结果基本一致.通过研究能量损耗、电场分布和磁场分布揭示了吸波机理,分析表明该吸波体的宽频吸收效果源于三层结构产生的吸收带宽叠加.本文提出的吸波超材料具有良好的宽频吸收效果,尤其在低频范围吸波性能较佳,结合3D打印快速成型技术,可获得结构精细的三层吸波超材料,具有重要的实际应用价值和广阔的应用前景. 相似文献
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本文设计了一种具有准全向吸波特性的平板超材料吸波体,其准全向吸波特性是由超材料吸波单元的双面吸波、极化不敏感和宽入射角实现的.理论分析和仿真结果表明:该吸波体在6.18 GHz的确有一个双面吸波的吸收点,且吸收率对极化角和入射角均不敏感.提取的等效阻抗表明可以调节超材料的电磁响应使其在吸收频率处与自由空间阻抗匹配来抑制反射.仿真的能量损耗分布表明:该吸波体对电磁波的吸收主要源于基板的介质损耗;采用两种不同介质基板的设计可使前吸波体与后吸波体的耦合度明显降低、抑制耦合所导致的传输.该吸波体可能在许多领域具有
关键词:
准全向吸波
双面吸波
极化不敏感
宽入射角 相似文献
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仿真并实验验证了基于电磁谐振的极化无关透射吸收超材料吸波体, 该吸波体可以实现低频透射和高频吸收.实验测试结果表明, 该吸波体在6.77 GHz 吸收率峰值为83.6%, 半功率带宽为4.3%, 实现窄带强吸收.为进一步拓展该谐振型超材料吸波体的吸收带宽, 利用其低频透射特性, 将两个工作于不同频段的吸波体叠加在一起, 测试结果表明, 复合后超材料吸波体的半功率带宽可以增大到10.9%, 吸收率也略有增强. 该超材料吸波体设计简单, 具有较强的实用性和应用前景.
关键词:
极化无关
透射吸收
超材料吸波体 相似文献
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In this paper, a broadband metamaterial absorber is successfully designed by a three-dimensional structure. And the three-dimensional absorber is just obtained by a two-dimensional structure which rotates 90°along x-axis. The simulated results show that the absorption of the three-dimensional metamaterial absorber is much better than the two-dimensional absorber. Moreover, the absorber is polarization-sensitive for the incident electromagnetic waves due to the asymmetry of the structure. Compared with the Y-polarization wave, the proposed absorber can realize broadband absorption with greater than 90% from 355.6 to 737.7 THz for X-polarized wave. Finally, based on the analysis of the electric field and surface current distributions, it can demonstrate that the localized surface plasmons and dipoles resonances will play an important role in the broadband absorption. And we believe that the metamaterial absorber will have many potential applications in emitter and energy harvesting. 相似文献
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Experimental demonstration of terahertz metamaterial absorbers with a broad and flat high absorption band 总被引:2,自引:0,他引:2
We present the design, numerical simulations and experimental measurements of terahertz metamaterial absorbers with a broad and flat absorption top over a wide incidence angle range for either transverse electric or transverse magnetic polarization depending on the incident direction. The metamaterial absorber unit cell consists of two sets of structures resonating at different but close frequencies. The overall absorption spectrum is the superposition of individual components and becomes flat at the top over a significant bandwidth. The experimental results are in excellent agreement with numerical simulations. 相似文献
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Yahong Liu Shuai Gu Chunrong Luo Xiaopeng Zhao 《Applied Physics A: Materials Science & Processing》2012,108(1):19-24
The design, fabrication, and measurements of a broadband metamaterial absorber are reported. The proposed metamaterial absorber consists of circular metallic patches and a metallic ground plane separated by a dielectric layer. Increasing the number of metallic patches can broaden the frequency range when their resonances are closely packed together, thereby resulting in a broadband resonance. Experimental results show that the proposed absorber has high absorptivity, with a full width at half maximum absorption bandwidth of 2.8 GHz and the relative FWHM absorption bandwidth of 25.3?%. In addition, the absorber can operate at a wide range of incident angles under both transverse electric and transverse magnetic polarizations. 相似文献
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Yongzhi Cheng Helin Yang Zhengze Cheng Nan Wu 《Applied Physics A: Materials Science & Processing》2011,102(1):99-103
In this paper, we present a polarization-insensitive metamaterial (MM) absorber which is composed of the dielectric substrate
sandwiched with split-ring-cross resonator (SRCR) and continuous metal film. The MM absorber is not limited by the quarter-wavelength
thickness and can achieve near-unity absorbance by properly assembling the sandwiched structure. Microwave experiments demonstrate
the maximum absorptivity to be about 99% around 10.91 GHz for incident wave with different polarizations. The surface currents
distributions of the resonance structure are discussed to look into the resonance mechanism. Importantly, our absorber is
only 0.4 mm thick, and numerical simulations confirm that the MM absorber could achieve very high absorptivity at wide angles
of incidence for both transverse electric (TE) wave and transverse magnetic (TM) wave. The sandwiched structure is also suitable
for designing of a THz and even higher frequency MM absorber, and simulations demonstrate the absorption of 99% at 1.105 THz. 相似文献
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Arising from the proposed Transmission Line(TL) model for ERR and wire structure, a TL model for a metamaterial absorber is proposed. The S-parameters obtained by this TL model demonstrate the same shapes as the simulation. An investigation of the TL model and average absorption power densities shows that the metamaterial absorber does not simply convert the electromagnetic wave into thermal energy, but concen- trate the electromagnetic wave into a small space where it is finally absorbed. This suggests that the metamaterial absorber can be applied to solar cells for the purpose of light trapping. 相似文献
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利用金属线单元组合法, 仿真设计并制作了一种在通信频段(0.8-3GHz)的双向多频超材料吸波器. 仿真与实验结果表明: 该吸波器对于不同极化和宽角度入射的电磁波有三个稳定的吸波频点, 分布在2.04GHz, 2.34GHz和2.65GHz, 吸收率分别达到92.3%, 95.3%和94.7%. 该吸波器设计简单、灵活性强、吸收效果好、易于加工, 为通信领域的电磁屏蔽或抗电磁干扰提供了新的方法.
关键词:
超材料
双向多频吸收
极化不敏感
宽角度入射 相似文献