2004
DOI: 10.1109/tps.2004.827596
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Reflections in Gyrotrons With Axial Output

Abstract: Influence of reflections on operation of gyrotrons with axial output is studied both theoretically and experimentally. By way of example the Fukui large orbit gyrotron with a permanent magnet operating in third harmonic at frequency 89 GHz is considered. In the case of strong reflection (= 0 6), extreme sensitivity of output power on the reflection phase is found. A qualitative agreement between theory and experiment is observed.

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Cited by 21 publications
(6 citation statements)
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References 8 publications
(7 reference statements)
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“…For high-power gyrotrons used for plasma heating for fusion applications, the reflections could stem from the output window, the transmission line between the gyrotron and the plasma, or by the first layer of the plasma itself [3]. Reflections can be favorable for gyrotron operation when they are controlled and limited, and have been shown to increase the rf output power [4,5], lock the gyrotron oscillation frequency [6], decrease the sensitivity of the radiation frequency to variation of the magnetic field [2], extend the frequency range by exciting different axial modes [7,8], and suppress parasitic modes [9]. However, when not controlled, even a limited amount of reflection can lead to a complete loss of oscillation by driving the gyrotron to a non-stationary or chaotic phase or into unstable operation in an undesired mode.…”
Section: Introductionmentioning
confidence: 99%
“…For high-power gyrotrons used for plasma heating for fusion applications, the reflections could stem from the output window, the transmission line between the gyrotron and the plasma, or by the first layer of the plasma itself [3]. Reflections can be favorable for gyrotron operation when they are controlled and limited, and have been shown to increase the rf output power [4,5], lock the gyrotron oscillation frequency [6], decrease the sensitivity of the radiation frequency to variation of the magnetic field [2], extend the frequency range by exciting different axial modes [7,8], and suppress parasitic modes [9]. However, when not controlled, even a limited amount of reflection can lead to a complete loss of oscillation by driving the gyrotron to a non-stationary or chaotic phase or into unstable operation in an undesired mode.…”
Section: Introductionmentioning
confidence: 99%
“…При отсутствии фазовой нелинейности (β ′′ 1 ) свойства собственных частот были исследованы в [15]. Аналогичное уравнение (7) можно получить для частоты второй моды. На рис.…”
Section: основные уравнения и результаты их анализаunclassified
“…При достаточно малых ρ 1 эта зависимость является однозначной (кривая 1). При росте коэффициента отражения число корней уравнения (7), то есть число собственных частот, увеличивается. Соответственно зависимость ω 1 (ψ 1 ) становится неоднозначной (кривая 2).…”
Section: основные уравнения и результаты их анализаunclassified
“…By placing different reflectors beyond the window and changing the distance between them and the window, one can vary both the magnitude and the phase of the reflection coefficient (see Ref. 7). This simplified scheme might be inaccurate in a real gyrotron, in which, in order to diminish reflection effects, the window can be The output power corresponding to B = 6.86 T is plotted with dashed lines for R el = 9.8 mm, with dots for R el = 9.9 mm and with solid lines for R el = 10.0 mm.…”
Section: Possible Experimentsmentioning
confidence: 99%