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1.
结合超宽带缝隙天线和分形结构的优点,设计了一种具有陷波特性的超宽带分形缝隙天线.选择E形缝隙结构,并在缝隙下边缘采用树状分形,构造半波长谐振结构,实现了天线的陷波功能,有效地避免了超宽带频带范围内的系统干扰.给出了天线设计的总体思路,通过理论分析和仿真测试,对天线的阻抗特性、增益进行了研究.结果表明,该陷波天线的阻抗频带为3 GHz ~12 GHz,在5 GHz~6.25 GHz频带内具有陷波特性.同时,分形结构的引入极大地缩小了天线的尺寸.  相似文献   

2.
设计了一款新型的具有陷波特性的超宽带单极子天线。该天线的带宽为3. 1 ~ 12. 0 GHz,通过在矩 形辐射贴片上制作出对称的梯形结构、中心加载倒C 形缝隙、矩形开槽,并将窄矩形接地板切除两个边角,制作矩形 开槽结构,使得天线在3. 3 ~5. 35 GHz 频段产生陷波特性。该天线结构紧凑,尺寸仅为20 mm×25 mm×1. 0 mm。建 立天线模型,并对其进行仿真和优化。研究表明,天线在WiMAX 频段、C 波段、数字微波通信、大容量微波通信和部 分WLAN 等多个频段产生良好的陷波特性,且在工作频段内有良好的性能和辐射方向特性。  相似文献   

3.
设计了一种小型三陷波平面超宽带天线,通过在天线的辐射贴片上加载U形缝隙、在接地板上开一对对称的L形缝隙和引入寄生条带,使得天线在3.2~3.6GHz、3.7~4.3GHz和5.3~6GHz频段内实现频率阻断。利用仿真软件研究了U形缝隙、L形缝隙和寄生条带对陷波特性的影响,并对所设计的超宽带天线进行了制作和测量。结果显示,该天线在工作频段2.8~10.6GHz内具有良好的辐射方向特性,能广泛应用于超宽带系统。  相似文献   

4.
廖银霜  王代强 《电讯技术》2021,61(5):640-645
为了在所需的多个陷波频带中获得额外的谐振频率,设计了一种具有五陷波特性的超宽带单极子天线,天线包括蚀刻了两个不封闭口字型槽的秤砣形贴片、矩形微带馈电线、缺陷接地板和两个类U形谐振器.将两个类U形谐振器耦合在馈电线附近,与辐射贴片上蚀刻的两个槽及缺陷接地板共同实现五陷波特性.该天线工作带宽为3.01~12 GHz,有效滤除了WiMAX通信频段(3.73~3.89 GHz)、C频段卫星通信系统(4.25~4.9 GHz)、无线局域网通信频段(5.51~5.83 GHz)、INSAT(Indian National Satellite System)频段(6.77~7.32 GHz)和ITU 8GHz频段(8.13~8.38 GHz)的干扰,且天线在通带频段内五个陷波特性和方向性结果均吻合良好.  相似文献   

5.
为避免窄带通信系统对超宽带(ultra-wideband,UWB)系统的干扰冲突,提出一款具有三陷波特性的类Sierpinski分形UWB天线.辐射贴片采用圆环与五角星形嵌套迭代的2阶类Sierpinski分形结构,并采用缺陷地结构接地板以实现良好的UWB特性.通过在分形结构的上部添加对称倒L形开路枝节,在微带馈线两侧添加对称L形开路枝节,并在馈线处刻蚀倒π形窄缝隙产生了4.5~4.8 GHz、7.2~7.8 GHz和8.0~8.5 GHz三个频段的陷波特性.仿真和实测结果表明,天线在3.1~18.1 GHz的频段内,可有效抑制国际卫星波段、X卫星波段和国际电信联盟波段等窄带系统的干扰.该天线除滤波频段内,在通带频段内有较稳定的增益和全向辐射特性,可用于各种UWB系统中.  相似文献   

6.
为避免窄带通信系统对超宽带(ultra-wideband,UWB)系统的干扰冲突,提出一款具有三陷波特性的类Sierpinski分形UWB天线.辐射贴片采用圆环与五角星形嵌套迭代的2阶类Sierpinski分形结构,并采用缺陷地结构接地板以实现良好的UWB特性.通过在分形结构的上部添加对称倒L形开路枝节,在微带馈线两侧添加对称L形开路枝节,并在馈线处刻蚀倒π形窄缝隙产生了4.5~4.8 GHz、7.2~7.8 GHz和8.0~8.5 GHz三个频段的陷波特性.仿真和实测结果表明,天线在3.1~18.1 GHz的频段内,可有效抑制国际卫星波段、X卫星波段和国际电信联盟波段等窄带系统的干扰.该天线除滤波频段内,在通带频段内有较稳定的增益和全向辐射特性,可用于各种UWB系统中.  相似文献   

7.
吴玲  夏应清  曹霞 《压电与声光》2017,39(5):794-796
设计了一种紧凑的具有三陷波特性的超宽带天线。天线采用渐变微带线馈电,并通过矩形加半圆的辐射单元和半圆形地板来实现超宽带。通过在辐射单元上刻蚀对称的L形槽和圆环形槽,来实现在WLAN/WiMAX的陷波特性;在渐变微带馈线两侧增加对称的C形谐振器来达到在X频段的陷波特性。实验结果表明,天线在2.68~13GHz频段内电压驻波比小于2,同时在3.1~3.8GHz,5~5.9GHz,7.25~7.85GHz频段内有陷波抑制作用,且具有良好的辐射特性。天线具有较小的几何尺寸,仅为20mm×30mm。  相似文献   

8.
余明 《通讯世界》2014,(5):26-27
针对超宽带通信系统(3.1~10.6GHz)与WLAN工作频段(5.15~5.825GHz)之间存在的电磁干扰,本文提出了一种小型化陷波超宽带天线。该天线结构简单,体积较小,陷波特性良好。通过在介质板上侧的金属地板刻蚀C形槽缝可以使天线在5.15~5.825GHz频段实现良好的陷波特性,而且调节C形槽缝的长度可以调节阻带的频段。研究结果表明,该天线的辐射特性良好,能够广泛应用于超宽带通信系统。  相似文献   

9.
提出了一款紧凑型多陷波特性超宽带天线,该天线由圆形贴片和改进的接地板组成。采用在辐射贴片上开两个圆弧状U形槽和接地板上开一个U形窄缝隙的结构使其具有多陷波特性。天线的体积仅为32 mm′25 mm′1.6 mm,结构紧凑。仿真与测试结果表明:该天线工作带宽为2.8 ~ 16 GHz,实现了3.2~3.8 GHz、4.5~5.5 GHz 和7.2~8.6 GHz 3个频段的陷波特性,有效阻隔了WiMAX(3.3~ 3.6 GHz)、大容量微波通信频段(4.5~5 GHz)、部分WLAN(5.1~5.35 GHz)、X波段(7.25~7.75 GHz)和国际电信联盟(ITU)波段(8.01~8.5 GHz)窄带信号的干扰。除陷波频段外该天线具有良好性能和辐射方向性,更适合应用于超宽带系统。  相似文献   

10.
设计了带三角形槽梯形辐射元和阶梯接地面的30 mm×30 mm印制单极超宽带天线原型.实验结果表明,原型天线驻波比小于2的阻抗带宽为2.8 GHz~12.81 GHz,频带内天线具有全向辐射特性,增益变化平坦,相位中心稳定.通过对原型天线振子体的缝隙加载,实现了具有带阻特性的陷波超宽带天线,其驻波比大于3的陷波频带为4.8 GHz~6.0 GHz,陷波频带内最高增益抑制为9 dB,而其他频段性能与原型天线基本一致.  相似文献   

11.
Waveguide multilayer optical card (WMOC) is a novel storage device of three-dimensional optical information. An advanced readout system fitting for the WMOC is introduced in this paper. The hardware mainly consists of the light source for reading, WMOC, motorized stages addressing unit, microscope imaging unit, CCD detecting unit and PC controlling & processing unit. The movement of the precision motorized stage is controlled by the computer through Visual Basic (VB) language in software. A control panel is also designed to get the layer address and the page address through which the position of the motorized stages can be changed. The WMOC readout system is easy to manage and the readout result is directly displayed on computer monitor.  相似文献   

12.
IntroductionNanoimprint Lithography is a well-acknowl-edged low cost, high resolution, large area pattern-ing process. It includes the most promising methods,high-pressure hot embossing lithography (HEL) [2],UV-cured imprinting (UV-NIL) [3] and micro contactprinting (m-CP, MCP) [4]. Curing of the imprintedstructures is either done by subsequent UV-lightexposure in the case of UV-NIL or by cooling downbelow the glass transition temperature of the ther-moplastic material in case of HEL…  相似文献   

13.
The collinearly phase-matching condition of terahertz-wave generation via difference frequency mixed in GaAs and InP is theoretically studied. In collinear phase-matching, the optimum phase-matching wave hands of these two crystals are calculated. The optimum phase-matching wave bands in GaAs and lnP are 0.95-1.38μm and 0.7-0.96μm respectively. The influence of the wavelength choice of the pump wave on the coherent length in THz-wave tuning is also discussed. The influence of the temperature alteration on the phase-matching and the temperature tuning properties in GaAs crystal are calculated and analyzed. It can serve for the following experiments as a theoretical evidence and a reference as well.  相似文献   

14.
Composition dependence of bulk and surface phonon-polaritons in ternary mixed crystals are studied in the framework of the modified random-element-isodisplacement model and the Bom-Huang approximation. The numerical results for Several Ⅱ - Ⅵ and Ⅲ- Ⅴ compound systems are performed, and the polariton frequencies as functions of the compositions for ternary mixed crystals AlxGa1-xAs, GaPxAS1-x, ZnSxSe1-x, GaAsxSb1-x, GaxIn1-xP, and ZnxCd1-xS as examples are given and discussed. The results show that the dependence of the energies of two branches of bulk phonon-polaritons which have phonon-like characteristics, and surface phonon-polaritons on the compositions of ternary mixed crystals are nonlinear and different from those of the corresponding binary systems.  相似文献   

15.
A doping system consisting of NPB and PVK is employed as a composite hole transporting layer (CHTL). By adjusting the component ratio of the doping system, a series of devices with different concentration proportion of PVK : NPB are constracted. The result shows that doping concentration of NPB enhances the competence of hole transporting ability, and modifies the recombination region of charge as well as affects the surface morphology of doped film. Optimum device with a maximum brightness of 7852 cd/m^2 and a power efficiency of 1.75 lm/W has been obtained by choosing a concentration proportion of PVK : NPB at 1:3.  相似文献   

16.
An insert layer structure organic electroluminescent device(OLED) based on a new luminescent material (Zn(salen)) is fabricated. The configuration of the device is ITO/CuPc/NPD/Zn(salen)/Liq/LiF/A1/CuPc/NPD/Zn(salen)/Liq/LiF/A1. Effective insert electrode layers comprising LiF(1nm)/Al(5 nm) are used as a single semitransparent mirror, and bilayer cathode LiF(1 nm)/A1(100 nm) is used as a reflecting mirror. The two mirrors form a Fabry-Perot microcavity and two emissive units. The maximum brightness and luminous efficiency reach 674 cd/m^2 and 2.652 cd/A, respectively, which are 2.1 and 3.7 times higher than the conventional device, respectively. The superior brightness and luminous efficiency over conventional single-unit devices are attributed to microcavity effect.  相似文献   

17.
Due to variable symbol length of digital pulse interval modulation(DPIM), it is difficult to analyze the error performances of Turbo coded DPIM. To solve this problem, a fixed-length digital pulse interval modulation(FDPIM) method is provided. The FDPIM modulation structure is introduced. The packet error rates of uncoded FDPIM are analyzed and compared with that of DPIM. Bit error rates of Turbo coded FDPIM are simulated based on three kinds of analytical models under weak turbulence channel. The results show that packet error rate of uncoded FDPIM is inferior to that of uncoded DPIM. However, FDPIM is easy to be implemented and easy to be combined, with Turbo code for soft-decision because of its fixed length. Besides, the introduction of Turbo code in this modulation can decrease the average power about 10 dBm, which means that it can improve the error performance of the system effectively.  相似文献   

18.
It is a key problem to accurately calculate beam spots' center of measuring the warp by using a collimated laser. A new method, named double geometrical center method (DGCM), is put forward for the first time. In this method, a plane wave perpendicularly irradiates an aperture stop, and a charge couple device (CCD) is employed to receive the diffraction-beam spots, then the geometrical centers of the fast and the second diffraction-beam spots are calculated respectively, and their mean value is regarded as the center of datum beam. In face of such adverse instances as laser intension distributing defectively, part of the image being saturated, this method can still work well. What's more, this method can detect whether an unacceptable error exits in the courses of image receiving, processing and calculating. The experimental results indicate the precision of this method is high.  相似文献   

19.
High purity organic-tantalum precursors for thin film ALD TaN were synthesized and characterized.Vapor pressure and thermal stability of these precursors were studied.From the vapor pressure analysis,it was found that TBTEMT has a higher vapor pressure than any other published liquid TaN precursor,including TBTDET,TAITMATA,and IPTDET.Thermal stability of the alkyl groups on the precursors was investigated using a 1H NMR technique.The results indicated that the tertbutylimino group is the most stable group on TBTDET and TBTEMT as compared to the dialkylamido groups.Thermal stability of TaN precursors decreased in the following order:TBTDET > PDMAT > TBTEMT.In conclusion,precursor vapor pressure and thermal stability were tuned by making slight variations in the ligand sphere around the metal center.  相似文献   

20.
In order to diagnose the laser-produced plasmas, a focusing curved crystal spectrometer has been developed for measuring the X-ray lines radiated from a laser-produced plasmas. The design is based on the fact that the ray emitted from a source located at one focus of an ellipse will converge on the other focus by the reflection of the elliptical surface. The focal length and the eccentricity of the ellipse are 1350 mm and 0.9586, respectively. The spectrometer can be used to measure the X- ray lines in the wavelength range of 0.2-0.37 nm, and a LiF crystal (200) (2d = 0.4027 nm) is used as dispersive element covering Bragg angle from 30° to 67.5°. The spectrometer was tested on Shengnang- Ⅱ which can deliver laser energy of 60-80 J/pulse and the laser wavelength is 0.35 μm. Photographs of spectra including the 1 s2p ^1P1-1s^2 ^1S0 resonance line(w), the 1s2p ^3P2-1s^2 1S0 magnetic quadrupole line(x), the 1s2p ^3P1-1 s^2 ^1S0 intercombination lines(y), the 1 s2p ^3S~1-1 s^2 ^1S0 forbidden line(z) in helium-like Ti Ⅹ Ⅺ and the 1 s2s2p ^2P3/2-1 s622s ^2S1/2 line(q) in lithium-like Ti Ⅹ Ⅹhave been recorded with a X-ray CCD camera. The experimental result shows that the wavelength resolution(λ/△ 2) is above 1000 and the elliptical crystal spectrometer is suitable for X-ray spectroscopy.  相似文献   

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