共查询到19条相似文献,搜索用时 140 毫秒
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波导间缝隙的互耦会严重降低高功率微波宽边纵缝波导缝隙阵的宽角扫描能力。设计了一L波段高功率宽边纵缝波导缝隙阵,在阵列波导间设计扼流槽结构抑制缝隙互耦。数值模拟结果表明,没有扼流槽结构的阵列波束扫描增益下降3 dB的角度为24.7°,具有扼流结构的阵列扫描增益下降3 dB的角度为33°。同时扼流结构还可以明显改善阵列的有源反射系数,有扼流结构的阵列有源VSWR≤3的带宽为6.6%,而没有扼流结构的阵列有源VSWR≤3的带宽为5.0%。数值模拟结果还表明,波束扫描时(扫描角35°),阵列功率容量可达到957 MW, 比阵列无波束扫描时(1.008 GW)稍低一点。 相似文献
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波导间缝隙的互耦会严重降低高功率微波宽边纵缝波导缝隙阵的宽角扫描能力。设计了一L波段高功率宽边纵缝波导缝隙阵,在阵列波导间设计扼流槽结构抑制缝隙互耦。数值模拟结果表明,没有扼流槽结构的阵列波束扫描增益下降3dB的角度为24.7°,具有扼流结构的阵列扫描增益下降3dB的角度为33°。同时扼流结构还可以明显改善阵列的有源反射系数,有扼流结构的阵列有源VSWR≤3的带宽为6.6%,而没有扼流结构的阵列有源VSWR≤3的带宽为5.0%。数值模拟结果还表明,波束扫描时(扫描角35°),阵列功率容量可达到957 MW,比阵列无波束扫描时(1.008GW)稍低一点。 相似文献
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隐埋波导耦合集成化激光器模拟设计 总被引:1,自引:0,他引:1
本文设计了一种利用隐埋波导耦合的集成化GaAs/GaAlAs单模激光器。并从四层不对称波导的基本电场方程及其本征方程出发,用计算机模拟方法,计算出该集成型激光器结构参数之间的关系,文中还讨论了在不同a、h(y)、D条件下基侧模的最小隐埋波导宽度W,波导中心厚度h,有效隐埋波导宽度W_(off)与横向光限制的关系.在模拟计算基础上,导出了四层不对称波导的归一化有效折射率b和限制Г_x因子的近似表示式,并得出该激光器最佳结构参数. 相似文献
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驻波测量线的槽波谐振实验及其分析戚家福(郑州大学物理系)为测绘出沿线驻波分布图形,要在波导测量线的宽边(a边)上开有与传输线轴平行的狭窄槽缝,所开槽缝的位置不应影响传输线内原来的场分布情况,因此,要求槽缝开在a边的中线位置.如果槽缝的位置有偏歪,由于... 相似文献
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根据TE0模光波导的本征场分布、瑞利索末菲标量衍射积分公式和激励源与光波导耦合的匹配效率公式,给出光波导端面衍射和耦合的归一化发射系数和接收系数计算公式,推导出光波导端面非接触耦合的耦合效率计算公式。光波导模场分布采用高斯函数近似表达,给出简洁的计算光波导端面非接触耦合的耦合效率函数表达式。最后,基于星形光波导耦合器结构参量的特点,将累加运算采用积分运算近似表达,给出星形光波导耦合器接收光波导总的接收效率与耦合器基本参量的关系,阐明了星形光波导耦合器的耦合特性。 相似文献
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利用机械调节波导宽边尺寸可变化波导波长,从而实现变频波束扫描相同的效果,针对窄边辐射波导行波阵的波束扫描特性进行了分析,以实现宽角波束扫描为目标,着重分析了不同辐射缝隙间距下变化宽边所能得到的最大波束扫描范围。设计了通过变化宽边尺寸实现宽角扫描的X波段窄边辐射波导缝隙阵,设计波束扫描范围指向波导馈入端,避开阵列法向辐射(此方向辐射效率较低),实现了29°的连续波束扫描范围,在波束扫描范畴内增益下降小于3 dB,辐射效率大于62%;设计缝隙宽度3 mm, 波导长度约1 m(缝隙数40),单根波导缝隙天线可实现高功率微波功率容量70 MW。 相似文献
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用横向等效网络方法分析了非线性平板波导中TM的色散关系和场分布.这种方法基于传输线理论,把非线性介质波导中复杂的电磁场问题等效于电路网络问题,用横向谐振技术得到色散方程.用数值方法计算了不同非线性机制下三层平板非线性波导中的TM波传输特性. 相似文献
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The characteristics of electromagnetic waves in a narrowing waveguide are investigated. A method for field analysis is developed based on the application of transverse modes parametrically dependent on the longitudinal coordinate. For a circular cross section waveguide, a system of equations for the wave amplitudes is obtained, the waves being coupled owing to a variable tilt of the walls. It is shown that in the adiabatic approximation, there exist independent eigenwaves whose structure reflects the field energy density variation due to the waveguide radius variation. A detailed analytical and numerical investigation of these fields has been carried out for a waveguide with a special profile of hypergeometric type. The applicability of the adiabatic approximation is studied and conversion of the fundamental mode into higher-order modes is assessed. The amplitudes of the higher-order modes are obtained using the Green function for ordinary differential equations. The region of the waveguide parameters is found where the higher-order mode amplitudes are not great and the adiabatic approximation is highly accurate. The dependence of the transmittance of a semi-infinite waveguide on the input radiation characteristics is obtained. It is established that the field amplitudes at the waveguide output strongly depend on the wavelength of the input radiation, on its transverse structure, and the waveguide profile steepness. The greatest output fields take place in the case of an abrupt dependence of the waveguide radius on the longitudinal coordinate. 相似文献
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Spectral and normal mode formulations for the three-dimensional field scattered by an object moving in a stratified medium are derived using full-field wave theory. The derivations are based on Green's theorem for the time-domain scalar wave equation and account for Doppler effects induced by target motion as well as source and receiver motion. The formulations are valid when multiple scattering between the object and waveguide boundaries can be neglected, and the scattered field can be expressed as a linear function of the object's plane wave scattering function. The advantage of the spectral formulation is that it incorporates the entire wave number spectrum, including evanescent waves, and therefore can potentially be used at much closer ranges to the target than the modal formulation. The normal mode formulation is more computationally efficient but is limited to longer ranges. For a monochromatic source that excites N incident modes in the waveguide, there will be roughly N2 distinct harmonic components in the scattered field. The Doppler shifts in the scattered field are highly dependent upon the waveguide environment, target shape, and measurement geometry. The Doppler effects are illustrated through a number of canonical examples. 相似文献
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设计了一种适用于窄带高功率微波源系统的紧凑型TEM-TE11模式转换器。该结构首先将同轴波导沿角向分区使微波在各分区内相位传播常数不同,然后将相位传播常数较大的分区进行横向折叠设计以缩短系统轴向长度。分区传播的微波在模式转换器末端相位差达到180时,合成同轴波导中TE11模式。为L波段磁绝缘振荡器设计了模式转换器,并采用数值仿真程序进行计算,在1.31 GHz中心频率上,模式转换器转换效率为95%;在1.23~1.40 GHz频率上,模式转换器效率大于90%,相对带宽13%。将模式转换器应用于磁绝缘振荡器,并测量了天线的定向辐射能力,所得结果与设计一致。 相似文献
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M. V. Markosyan A. A. Martirosyan A. K. Aharonyan V. H. Avetisyan 《Journal of Contemporary Physics (Armenian Academy of Sciences)》2018,53(3):194-201
The unusual paired slotted radiating structure of a circular waveguide is investigated when the wave of main mode H11 is propagating in it. This structure is constructed in such a way that the phenomenon of the polarization degeneration of wave with this mode is taken into account. In the waveguide cross-section, the centers of the paired half-wave transverse slots are spaced by an angle γ over both sides of the waveguide diametric line along the direction of polarization of the H11 mode. The radiation patterns at different spaced angles γ equal to 45°, 65°, and 72° as well as at the two-tiered location of such paired slots are investigated. The second tier is located on the distance equal to the half of the waveguide wavelength along the waveguide longitudinal axis. The pair slots of both tiers have the same γ angle but they are located at the opposite sides of the waveguide. The possibility is shown of synthesizing an omnidirectional radiation pattern by combination of the two-tiered structure with the opposite frontal slots and the two-tiered structure with the oppositely paired slots. 相似文献
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A compact and fabrication friendly polarization demultiplexer (P-DEMUX) is proposed and characterized to enable wavelength-division-multiplexing and polarization-division-multiplexing simultaneously. The proposed structure is composed of a polarization-selective microring resonator in ultrathin waveguide and two bus channels in the silicon nitride-silica-silicon horizontal slot waveguides. In the slot waveguide, the transverse electric (TE) mode propagates through the silicon layer, while the transverse magnetic (TM) mode is confined in the slot region. In the designed ultra-thin waveguide, the TM mode is cut-off. The effective indexes of the TE modes for ultrathin and slot waveguides have comparable values. Thanks for these distinguishing features, the input TE mode can be efficiently filtered through the ultra-thin microring at the resonant wavelength, while the TM mode can directly output from the through port. Simulation results show that the extinction ratio of the proposed P-DEMUX for TE and TM modes are 33.21 dB and 24.97 dB, and the insertion losses are 0.346 dB and 0.324 dB, respectively, at the wavelength of 1551.64 nm. Furthermore, the device shows a broad bandwidth ($>100$ nm) for an extinction ratio (ER) of $>20$ dB. In addition, the proposed P-DEMUX also has a good fabrication tolerance for the waveguide width variation of $-20$ nm$\le \Delta w_{\rm g}\le 20$ nm and the microring width variation of $-20$ nm$\le \Delta w_{\rm r}\le $20 nm for a low insertion loss of $<0.75$ dB and low ER of $<-18$ dB. 相似文献
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提出利用超材料吸波体减缩波导缝隙阵列天线带内雷达散射截面的设计方法. 设计具有超薄(厚度仅为0.01λ, λ为吸波体中心频率对应波长)、无表面损耗层和高吸波率的超材料吸波体, 将其加载到波导缝隙天线E面方向辐射缝隙间的金属表面上, 并与辐射缝隙保持一定的间距. 该加载方式没有破坏天线的口径馈电振幅分布, 并利用超材料吸波体对电磁波的强吸收特性降低了天线阵的结构模式项散射. 仿真和实验结果表明, 加载超材料吸波体后天线阵的反射系数、增益、波瓣宽度保持不变, 在x极化和y极化条件下, 波导缝隙阵列天线的带内雷达散射截面减缩量均在6 dB 以上, 且在-25°-+25°范围内天线雷达散射截面均有明显的减缩, 鼻锥方向减缩超过10 dB. 该研究成果对阵列天线雷达散射截面减缩具有重要的借鉴意义和工程应用价值. 相似文献
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Numerical analysis of surface plasmon nanocavities formed inthickness-modulated metal-insulator-metal waveguides 下载免费PDF全文
The enhancement characteristics of the local field in the
surface plasmon nanocavities are investigated numerically. The
cavity is constructed by placing a defect structure in the
thickness-modulated metal--insulator--metal waveguide Bragg gratings.
The characteristic impedance based transfer matrix method is used to
calculate the transmission spectra and the resonant wavelength of
the cavities with various geometric parameters. The
finite-difference time-domain method is used to obtain the field
pattern of the resonant mode and validate the results of the
transfer matrix method. The calculation and simulation results
reveal the existence of resonant wavelength shift and intensity
variation with structural parameters, such as the modulation period
of the gratings, the length and the width of the defect structure.
Both numerical analysis and theoretical interpretation on these
phenomena are given in details. 相似文献
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提出一种紧凑型偏振解复用器, 其中两条常规硅基波导作为输入/输出信号通道, 居于其中的槽式微环谐振腔用于偏振态/波长选择组件. 采用全矢量频域有限差分法详细分析了硅基常规及槽波导的模式特性, 结果发现其横磁模的模场布及其有效折射率相似, 而其横电模相应的特性则差异明显, 结果输入横磁模能够在谐振工作波长下从下路端口输出, 而输入横电模与微环耦合可以忽略, 直接从直通端口输出, 从而实现两偏振态的高效分离. 采用全矢量时域有限差分法详细分析了该偏振解复用器的光波传输特性, 结果表明, 当微环半径为3.489 μm时, 在1.55 μm工作波长下, 横磁模与横电模的消光比与插入损耗分别为 ~ 26.12 (36.67) dB与 ~ 0.49 (0.09) dB. 另外, 论文详细讨论了器件关键结构参数的制作容差, 并给出了输入模场在器件中的传输演变情况. 相似文献