2019
DOI: 10.1109/ted.2019.2894537
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Design and Experiment of a High Average Power Ku-Band TE01 Mode Gyro-TWT

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Cited by 17 publications
(2 citation statements)
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“…7a and 8 it becomes evident that the operating TE 17,2 mode of the 0.39-THz second-harmonic gyrotron dominates over the remaining competing modes in a wide frequency range, provided that the loss tangent tan  is increased up to 0.07 for the dielectric insert with 9 r   and 1.3 i R  mm. In this case, the dielectric-loaded cavity for the 0.39-THz second-harmonic gyrotron meets the design goal, even though the increased dielectric losses still remain much lower than those usually employed to suppress parasitic modes in interaction structures and beam tunnels of gyro-devices [41,42,50,51].…”
Section:  mentioning
confidence: 98%
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“…7a and 8 it becomes evident that the operating TE 17,2 mode of the 0.39-THz second-harmonic gyrotron dominates over the remaining competing modes in a wide frequency range, provided that the loss tangent tan  is increased up to 0.07 for the dielectric insert with 9 r   and 1.3 i R  mm. In this case, the dielectric-loaded cavity for the 0.39-THz second-harmonic gyrotron meets the design goal, even though the increased dielectric losses still remain much lower than those usually employed to suppress parasitic modes in interaction structures and beam tunnels of gyro-devices [41,42,50,51].…”
Section:  mentioning
confidence: 98%
“…Such a rod can be fabricated from commercial AlN-SiC (or BeO-SiC) ceramics, which can possess loss tangent in the wide range from 0.001 to 0.5 depending on volume fraction of SiC [34,39,40]. Benefits of these ceramics are vacuum compatibility and exceptionally high thermal conductivity, which make such dielectrics suitable for use in high-power vacuum devices [41,42]. The radius of the lossy dielectric rod must be selected sufficiently small to have only a slight effect on the operating mode.…”
Section:  mentioning
confidence: 99%