Quasi-optical mode converter for a high power TE8,3-mode gyrotron

We successfully developed a Gyrotron HS-III (28-GHz/400-kW/5-s) for electron cyclotron resonance heating in a spherical tokamak EXL-50, which operated in the TE8,3 mode. An internal quasi-optical-mode converter was designed to separate the spent electron beam from the outgoing power and convert the...

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Published inAIP advances Vol. 12; no. 7; pp. 075116 - 075116-7
Main Authors Huang, Qili, Hu, Linlin, Ma, Guowu, Zhuo, Tingting, Sun, Dimin, Zhang, Luqi, Guo, Jun, Hu, Peng, Jiang, Yi, Chen, Hongbin, Jin, Xiao
Format Journal Article
LanguageEnglish
Published Melville American Institute of Physics 01.07.2022
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Abstract We successfully developed a Gyrotron HS-III (28-GHz/400-kW/5-s) for electron cyclotron resonance heating in a spherical tokamak EXL-50, which operated in the TE8,3 mode. An internal quasi-optical-mode converter was designed to separate the spent electron beam from the outgoing power and convert the operating mode to a fundamental Gaussian wave beam. The particle swarm optimization algorithm was used to reduce diffraction loss from the launcher in such a low-frequency band. This enabled us to optimize the perturbation distribution of the launcher and beam waist of the target function to obtain the largest possible scalar correlation coefficient. The launcher was followed by three mirrors: one quasi-parabolic mirror and two phase-correcting mirrors. These were also optimized based on the scalar diffraction theory and Katsenelenbaum–Semenov algorithm to allow us to change the beam direction and increase the purity of the Gaussian output beam. Simulation results revealed a transmission efficiency of 96% and vector Gaussian mode purity of 99.8% at the window plane.
AbstractList We successfully developed a Gyrotron HS-III (28-GHz/400-kW/5-s) for electron cyclotron resonance heating in a spherical tokamak EXL-50, which operated in the TE8,3 mode. An internal quasi-optical-mode converter was designed to separate the spent electron beam from the outgoing power and convert the operating mode to a fundamental Gaussian wave beam. The particle swarm optimization algorithm was used to reduce diffraction loss from the launcher in such a low-frequency band. This enabled us to optimize the perturbation distribution of the launcher and beam waist of the target function to obtain the largest possible scalar correlation coefficient. The launcher was followed by three mirrors: one quasi-parabolic mirror and two phase-correcting mirrors. These were also optimized based on the scalar diffraction theory and Katsenelenbaum–Semenov algorithm to allow us to change the beam direction and increase the purity of the Gaussian output beam. Simulation results revealed a transmission efficiency of 96% and vector Gaussian mode purity of 99.8% at the window plane.
Author Jin, Xiao
Ma, Guowu
Huang, Qili
Hu, Linlin
Hu, Peng
Chen, Hongbin
Sun, Dimin
Zhuo, Tingting
Zhang, Luqi
Jiang, Yi
Guo, Jun
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Snippet We successfully developed a Gyrotron HS-III (28-GHz/400-kW/5-s) for electron cyclotron resonance heating in a spherical tokamak EXL-50, which operated in the...
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StartPage 075116
SubjectTerms Algorithms
Converters
Correlation coefficients
Cyclotron resonance devices
Diffraction theory
Electron beams
Electron cyclotron resonance
Gaussian beams (optics)
Launchers
Low frequencies
Particle swarm optimization
Perturbation
Purity
Transmission efficiency
Wave diffraction
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Title Quasi-optical mode converter for a high power TE8,3-mode gyrotron
URI http://dx.doi.org/10.1063/5.0096003
https://www.proquest.com/docview/2687900558
https://doaj.org/article/733e2be3d3e749df8bb998268e63384a
Volume 12
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