二维五筒型光子晶体结构的提出

设计了一种二维五筒型晶格光子晶体的结构,利用PWE方法计算并仿真了该结构的能带分布,分析出了其带隙分布与介质柱介电常数和占空比的关系,总结出了能带与两者之间的变化规律.通过与方形、三角和六角晶格结构的能带分布比较,得到了四种晶格具有最大完全带隙时的参数,发现五筒型光子晶体结构具有最大的完全带隙,为进一步光子晶体的实验制...     

结构参数对二维光子晶体完全带隙影响的研究

完全带隙的分布决定了二维光子晶体特性,采用平面波展开法对三角形结构二维光子晶体的带隙随结构参数的变化进行了研究,计算结果表明:对于空气孔型二维光子晶体,当介质比εb/εa=13时,最佳归一化半径为r/a=0.48,此时完全带隙底宽度最大,最大完全带隙的宽度△(?)a/2πc=0.0902;当归一化半径固定时, 完全带隙的宽度随介质比的变大而增加。     

单分散性sio2胶体微球自组装光子晶体的实验研究

光子晶体是一种周期性电介质材料,具有光子带隙和光子局域等一系列优异的光学特性。制备了多种不同直径的单分散二氧化硅胶体微球,采用垂直沉积法将不同直径,以及同一直径不同浓度的二氧化硅胶体微球自组装成多种光子晶体薄膜,并用扫描电子显微镜和紫外—可见—近红外分光光度计对其微观结构和光学特性进行了表征,结果表明所得晶体薄膜具有三维有序结构,其表面存点、线缺陷。自组装得到的光子晶体薄膜存在明显的光子带隙特征,带隙位置与二氧化硅胶体微球直径有关,带隙中心波长与理论值一致。随着二氧化硅胶体微球浓度的增加,光子带隙深度增加,特性更好,但是,当浓度大于10%时,光子带隙的深度反而减小。     

光子晶体的研究进展

光子晶体是一种具有光子带隙的周期性电介质结构,落在光子带隙中的光不能传播.由于其独特的调节光子传播状态的功能,成为实现光通讯和光子计算机的基础.光子晶体的制备是发展光子晶体的关键,而可见光和近红外波段光子晶体的制备更是难点.本文阐述了光子晶体的概念及其特性后,分别介绍了光子晶体的实验研究和应用研究.实验研究重点介绍了光子晶体的制备方法.应用研究重点介绍了单模发光二极管光、光波导器件和微波天线等.     

光子晶体带隙法在溶液浓度测量中的应用

本文从光子晶体带隙理论出发,分析了相对带隙宽度与测量溶液浓度的之间的对应关系,提出了采用光子晶体平面波展开法测定牛奶浓度的新方案。通过研究以硅半导体材料为背景介质周期性排列空气孔圆柱构成的光子晶体,发现在高频率区域,二维三角晶格结构各向同性光子晶体的光子带隙随待测溶液百分浓度不同而单调变化的。这对浓度测量和高血糖患者的临床应用有一定的指导作用。     

结构参数对二维光子晶体完全带隙影响的研究

完全带隙的分布决定了二维光子晶体特性,采用平面波展开法对三角形结构二维光子晶体的带隙随结构参数的变化进行了研究,计算结果表明：对于空气孔型二维光子晶体,当介质比εb/εa=13时,最佳归一化半径为r/a=0.48,此时完全带隙底宽度最大,最大完全带隙的宽度△ωa/2πc=0.0902;当归一化半径固定时,完全带隙的宽度随介质比的变大而增加.     

1550nm处空芯光子晶体光纤带隙结构的研究

文章利用全矢量平面波法分析了二维三角结构空芯光子晶体光纤平面内和平面外存在的光子带隙的结构图.重点分析了课题组拉制的空芯光子晶体光纤,计算出了存在光子带隙的波长范围,发现在1550nm的光纤通讯窗口也存在光子带隙.通过理论计算这种光纤,发现随着包层的空气填充率、包层与空气孔两介质的相对折射率差的增大,带隙宽度也将随之增大.最后,说明了如何制备宽带隙的光子晶体光纤.     

变周期结构光子晶体的带隙研究

研究了变周期结构的光子晶体,即两种介质的厚度随单元数增加而变化,并对其光子能带特性进行了分析.研究发现,相对于周期性光子晶体,相同单元数的变周期结构的光子晶体具有更宽的光子能带带隙,且周期非线性变化比线性变化结构有更宽的光子带隙,这样对于同样宽的带隙的光子晶体,可采用较少单元数的变周期结构光子晶体,这一结果有助于光子晶体的广泛应用.     

复合型二维光子晶体的带隙展宽特性

选用时域有限分方法(FDTD)分析光子晶体带隙结构.选择两种不同晶格常数的二维光子晶体构成复合型二维光子晶体,计算了复合型光子晶体和组合光子晶体在近红外频段的带隙结构,结果表明,复合型二维光子晶体在近红外波频段的禁带宽度明显大于组合光子晶体禁带宽度.通过改变复合光子晶体的介电常数,实现其禁带向高频区或低频区移动.     

用平面波展开法计算二维方形光子晶体的带隙结构

用平面波展开法计算二维正方晶格光子晶体的带隙结构,对二维光子晶体的电磁波理论及周期介质中的Bloch波解进行了详细的推导,得出TE模和TM模下无缺陷时光子晶体的色散曲线,并设计了低频区域内具有较大带隙宽度的两种二维光子晶体的空间周期结构.经过大量的计算,发现硅中的空气柱型光子晶体在红外波段TE模和TM模存在重叠的绝对光子带隙,并分别研究了空气中的硅介质柱和硅中的空气柱的TM模带隙宽度随空气柱半径和填充比变化的规律.     

Ku-band stop filter implemented on a high resistivity silicon with inverted microstrip line photonic bandgap (PBG) structure

We have developed the inverted microstrip line photonic bandgap (IML-PBG) structure using the surface micro-machining technology on the high resistivity silicon (HRS) substrate. Because, when the IML was fabricated, the holes for removing a sacrificial layer were necessary, we have introduced these holes into the PBG structure for the Ku-band stop filter (BSF). Rectangular spiral PBG structure showed the notch characteristics and the array with suitable distance showed the stop band with under -20 dB from 15 to 19 GHz and under -3 dB pass-band loss.     

光子带隙结构在微带线中的应用

提出了一种用于微带线的光子带隙结构,该结构由在微带线的底板上光刻出成周期型的正方形环缝组成,对此结构进行了仿真.通过改变环缝的边长,可以看到它们具有不同的阻带特性.     

Low profile spiral antenna with PBG substrate

A novel spiral antenna backed on photonic bandgap (PBG) material is presented. It consists of a spiral radiator, a PBG substrate and a feed network; and exhibits a wider frequency bandwidth, larger ratio of front-to-back radiation level, and higher gain than a traditional spiral antenna with λ/4 spaced ground plate     

平面带隙结构在微波和毫米波集成电路中的应用

介绍了平面带隙结构在微波集成电路应用方面的最新进展。光子带隙(PBG)结构是具有带阻特性的周期结构,最初应用于光学领域,后来扩展到其他领域。目前从可见光到红外都有研究,在微波和毫米波频段也有应用。PBG结构可以采用金属、介质、铁磁或铁电物质植入衬底材料,或者直接由各种材料周期性排列而成。目前国内外所提出的光子带隙结构多种多样,一维和二维的平面带隙结构由于易于实现且便于集成,因而在微波毫米波集成电路中得到了广泛的应用。     

一种新颖的光子带隙平面螺旋天线

介绍了阿基米德螺旋天线的原理与设计方法,仿真了背腔式阿基米德螺旋天线,并与实际测试结果吻合;研究了一种新颖的光子带隙平面螺旋天线,这种天线用光子带隙代替金属反射腔作为反射面以得到单向波束,仿真与实验发现,光子带隙阿基米德螺旋天线的增益提高约有2dB,后瓣降低了10dB,在有效的工作带宽内天线的性能得到了改善.     

Large negative dispersion in square solid-core photonic bandgap fibers

In this paper, a Ge-doping square solid-core photonic bandgap (PBG) fiber is proposed and the effective index of defect mode is investigated. Simulations show that, at the starting wavelength of the defect mode, n/sub effd/ (the effective index of defect mode) changes rapidly due to the PBG effect, which induces large negative dispersion in fiber. This mechanism is different from the mode coupling case in dual-core concentric fibers, and the dispersion characteristic is more robust to structural deviations.     

A novel TEM waveguide using uniplanar compact photonic-bandgap(UC-PBG) structure

A novel waveguide using a photonic bandgap (PBG) structure is presented. The PBG structure is a two-dimensional square lattice with each cell consisting of metal pads and four connecting lines, which are etched on a conductor-backed Duroid substrate. This uniplanar compact PBG structure realizes a magnetic surface in the stopband and is used in the waveguide walls to provide magnetic boundary conditions. A relatively uniform field distribution along the cross section has been measured at frequencies from 9.4 to 10.4 GHz. Phase velocities close to the speed of light have also been observed in the stopband, indicating that TEM mode has been established. A recently developed quasi-Yagi antenna has been employed as a broad-band and efficient waveguide transition. Meanwhile, full-wave simulations using the finite-difference time-domain method provide accurate predictions for the characteristics of both the perfect magnetic conductor impedance surface and the waveguide structure. This novel waveguide structure should find a wide range of applications in different areas, including quasi-optical power combining and the electromagnetic compatibility testing     

PBG-excited split-mode resonator bandpass filter

Photonic bandgap structure is used as a design parameter for the fundamental passband in a split-mode microstrip square resonator. A defect in the PBG cells under the resonator, allows coupling between the two degenerate modes. A filter is designed at 2.2 GHz with good agreement between simulated and measured results     

Photonic bandgap formation and tunability in certainself-organizing systems

We describe the microfabrication and band structure of large scale three-dimensional (3D) photonic bandgap (PBG) materials based on self-organizing templates. The simplest of these templates is an fcc lattice of close-packed, weakly sintered spheres. Other templates include hcp and hexagonal AB₂ self-organizing photonic crystals. These photonic crystals may be converted into PEG materials by partially infiltrating the template with high refractive index semiconductors such as Si, Ge, or GaP and subsequently removing the template. The resulting “inverse opal” structure exhibits both a photonic pseudogap and a complete (3D) PBG in the near visible spectrum, spanning up to 15% of the gap center frequency. The local density of states (LDOS) for photons exhibits considerable variation from point to point in coordinate space and reveals large spectral gaps even in the absence of a PEG in the total density of states. These gaps in the LDOS may lead to novel effects in quantum and nonlinear optics when active atoms or molecules are placed within the PBG material. These effects include anomalous, low threshold nonlinear response, collective atomic switching, and low-threshold all-optical transistor action. When an optically birefringent nematic liquid crystal is infiltrated into the void regions of the “inverse” opal PBG material, the resulting composite material exhibits a completely tunable PBG. In particular, the 3D PBG can be completely opened or closed by applying an electric field which rotates the axis of the nematic molecules relative to the inverse opal backbone     

A novel uniplanar compact photonic bandgap power plane with ultra-broadband suppression of ground bounce noise

A novel /spl pi/-bridged photonic bandgap (PBG) power/ground planes is proposed with ultra-broadband suppression of the ground bounce noise(GBN) in the high-speed printed circuit boards. The S-parameters of the proposed low-period structures show that the novel uniplanar compact photonic bandgap (UC-PBG) structures could omni-directionally suppress the GBN in RF/analog circuits and digital circuits. The high omnidirectionally suppressions of the GBN for the proposed structure are validated both experimentally and numerically in the noise bandwidth from 300MHz to 6GHz, almost the whole noise band.