• Acta Physica Sinica
  • Vol. 69, Issue 6, 068401-1 (2020)
Xiao-Tong Guan1、2, Wen-Jie Fu2、*, Dun Lu2, Tong-Bin Yang2, Yang Yan2, and Xue-Song Yuan2
Author Affiliations
  • 1School of Physics, University of Electronic Science and Technology of China, Chengdu 610054, China
  • 2Terahertz Research Center, School of Electronic Science and Engineering, University of Electronic Science and Technology of China, Chengdu 610054, China
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    DOI: 10.7498/aps.69.20191222 Cite this Article
    Xiao-Tong Guan, Wen-Jie Fu, Dun Lu, Tong-Bin Yang, Yang Yan, Xue-Song Yuan. Design of second harmonic terahertz gyrotron cavity based on double confocal waveguide[J]. Acta Physica Sinica, 2020, 69(6): 068401-1 Copy Citation Text show less
    Cross section of quasi-optical waveguides in elliptic coordinate system: (a) Normal confocal waveguide; (b) double confocal waveguide.
    Fig. 1. Cross section of quasi-optical waveguides in elliptic coordinate system: (a) Normal confocal waveguide; (b) double confocal waveguide.
    Transverse geometry with the annular electron beam and electric field distributions of TE0, 11 mode in two types of quasi-optical waveguides: (a) Normal confocal waveguide; (b) double confocal waveguide.
    Fig. 2. Transverse geometry with the annular electron beam and electric field distributions of TE0, 11 mode in two types of quasi-optical waveguides: (a) Normal confocal waveguide; (b) double confocal waveguide.
    Mode spectrum in double confocal waveguide.
    Fig. 3. Mode spectrum in double confocal waveguide.
    Double confocal cavity: (a) Structural diagram; (b) axial field profile of TE0,11,1 mode.
    Fig. 4. Double confocal cavity: (a) Structural diagram; (b) axial field profile of TE0,11,1 mode.
    Beam-wave coupling factors as functions of electron beam radius Rb for different modes in double confocal waveguides.
    Fig. 5. Beam-wave coupling factors as functions of electron beam radius Rb for different modes in double confocal waveguides.
    Beam-wave coupling factors for TE0,11 mode in single and double confocal waveguide: (a) Radial distribution of coupling factor ; (b) azimuthal distribution of coupling factor Ls for an annular electron beam with Rb = 1.65 mm.
    Fig. 6. Beam-wave coupling factors for TE0,11 mode in single and double confocal waveguide: (a) Radial distribution of coupling factor ; (b) azimuthal distribution of coupling factor Ls for an annular electron beam with Rb = 1.65 mm.
    Calculated results of starting current Ist (V0 = 40 kV, α = 1.5, Rb = 1.65 mm): (a) For different modes in double confocal cavity; (b) for mode in double and single confocal cavity.
    Fig. 7. Calculated results of starting current Ist (V0 = 40 kV, α = 1.5, Rb = 1.65 mm): (a) For different modes in double confocal cavity; (b) for mode in double and single confocal cavity.
    Simulation results of output field Ex and Ey for double confocal cavity: (a) Time variation; (b) spectrum.
    Fig. 8. Simulation results of output field Ex and Ey for double confocal cavity: (a) Time variation; (b) spectrum.
    Simulation results of the distribution of electronic field Ex in double confocal cavity: (a) At output port; (b) at the xz plane (y = 0); (c) at the yz plane (x = 0).
    Fig. 9. Simulation results of the distribution of electronic field Ex in double confocal cavity: (a) At output port; (b) at the xz plane (y = 0); (c) at the yz plane (x = 0).
    Simulation results of the distribution of electronic field Ey in double confocal cavity: (a) At output port; (b) at the xz plane (y = 0); (c) at the yz plane (x = 0).
    Fig. 10. Simulation results of the distribution of electronic field Ey in double confocal cavity: (a) At output port; (b) at the xz plane (y = 0); (c) at the yz plane (x = 0).
    Simulation results for single confocal cavity: (a) Time variation of the output field Ex and Ey; (b) spectrum of the output field Ex.
    Fig. 11. Simulation results for single confocal cavity: (a) Time variation of the output field Ex and Ey; (b) spectrum of the output field Ex.
    Simulation results of output power for double confocal cavity and single confocal cavity.
    Fig. 12. Simulation results of output power for double confocal cavity and single confocal cavity.
    Expanded results of the output field Ex and Ey for double confocal cavity around 100 ns.
    Fig. 13. Expanded results of the output field Ex and Ey for double confocal cavity around 100 ns.
    截止端镜面半径Rc1/mm 直段镜面半径Rc2 /mm 输出端镜面半径Rc3 /mm 截止段长度L1 /mm 直段长度L2 /mm 输出段长度L3 /mm 镜面宽度2a /mm
    4.485.105.60917103.6
    Table 1. Design parameters of the proposed double confocal cavity.
    Xiao-Tong Guan, Wen-Jie Fu, Dun Lu, Tong-Bin Yang, Yang Yan, Xue-Song Yuan. Design of second harmonic terahertz gyrotron cavity based on double confocal waveguide[J]. Acta Physica Sinica, 2020, 69(6): 068401-1
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