Journal of Infrared and Millimeter Waves, Volume. 39, Issue 5, 567(2020)
Fig. 1. The configuration of the quasi-optical mode converter with a Denisov launcher. 1: Denisov launcher, 2~5: mirror system 6: output window
Fig. 4. (a) Variation of axial reflective angle
Fig. 5. Variation of structural parameter
Fig. 6. Variation of axial reflective angle
Fig. 7. Variation of structural parameter
Fig. 8. The The disturbance amplitude of Denisov launcher.in TE6.2 mode
Fig. 9. (a) The field distribution of Denisov launcher on the unrolled waveguide wall at 94 GHz in TE6,2 mode. The white line represents the cutting position (b) The 3D field distribution of Denisov launcher on the unrolled waveguide wall at 94 GHz in TE6,2 mode.
Fig. 10. The whole field distribution on quasi-optical mode converter at 94 GHz in TE6,2 mode.
Fig. 11. The field distribution on the output window at different frequency points from 93~95 GHz in TE6,2 mode.
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Hui-Qi BIAN, Chao-Hai DU, Shi PAN, Pu-Kun LIU.
Category: Millimeter Wave and Terahertz Technology
Received: Dec. 16, 2019
Accepted: --
Published Online: Dec. 29, 2020
The Author Email: Chao-Hai DU (duchaohai@pku.edu.cn), Pu-Kun LIU (pkliu@pku.edu.cn)