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220 GHz新型SIW-波导过渡结构的设计
引用本文:刘 军,于伟华,吕 昕. 220 GHz新型SIW-波导过渡结构的设计[J]. 太赫兹科学与电子信息学报, 2017, 15(3): 364-367
作者姓名:刘 军  于伟华  吕 昕
作者单位:Beijing Key Laboratory of Millimeter Wave and Terahertz Technology,Beijing University of Technology,Beijing 100081,China,Beijing Key Laboratory of Millimeter Wave and Terahertz Technology,Beijing University of Technology,Beijing 100081,China and Beijing Key Laboratory of Millimeter Wave and Terahertz Technology,Beijing University of Technology,Beijing 100081,China
摘    要:基片集成波导(SIW)既有波导的损耗低、品质因数高、功率容量大的特点,又兼具微带线的低剖面、尺寸小、易于与其他平面电路集成的优点,被广泛应用于微波电路设计之中。鉴于目前测试系统及级联都采用矩形波导端口,为实现对SIW元器件的测试及系统集成,须对SIW元器件进行过渡结构设计。采用三维高频电磁仿真软件仿真和优化,设计了一种新型SIW-波导过渡结构。仿真结果表明:该结构在205~225 GHz频段内,带内插入损耗在0.5~0.6 dB之间,回波损耗大于12 dB;背对背结构,插入损耗小于1.5 dB,回波损耗大于10 dB,相对带宽11.4%。

关 键 词:太赫兹;基片集成波导;过渡结构
收稿时间:2015-12-13
修稿时间:2016-02-09

Design of new type Substrate Integrated Waveguide-to-microstrip transition structure in 220 GHz
LIU Jun,YU Weihua and LYU Xin. Design of new type Substrate Integrated Waveguide-to-microstrip transition structure in 220 GHz[J]. Journal of Terahertz Science and Electronic Information Technology, 2017, 15(3): 364-367
Authors:LIU Jun  YU Weihua  LYU Xin
Abstract:Substrate Integrated Waveguide(SIW) has been widely used in microwave circuits because it bears the advantages of both waveguide and microstrip, such as low cost, high Q, compact size, and easy for fabrication, etc. In order to measure the scattering parameters of planar SIW components and realize system integration, it is necessary to develop the transition between SIW and rectangular metallic waveguide because most of the measurement systems are waveguide based. The transition between SIW and waveguide is designed and optimized by using High Frequency Structure Simulator(HFSS). The simulation results indicate that: in 205-220 GHz, the in-band insertion loss is between 0.5-0.6 dB, and the return loss is more than 12 dB; the back to back structure has less than 1.5 dB insertion loss and the return loss is more than 10 dB, the relative bandwidth is 11.4%.
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