1997
DOI: 10.1063/1.872133
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High efficiency cavity design of a 170 GHz gyrotron for fusion applications

Abstract: The design of high power, continuous wave ͑cw͒, 170 GHz gyrotron cavities is considered. The anticipated degradation of efficiency with beam velocity spread places a premium on the optimization of efficiency. For parameters of interest achievement of high efficiency requires utilization of a high quality cavity. Two options are considered: a barrel cavity and a long simple tapered cavity operating at low voltage. The cavities are examined for their sensitivity to velocity spread, their mode competition, and th… Show more

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Cited by 13 publications
(2 citation statements)
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“…¼ =T (T is the transient time of the electrons through the resonator) are considered in the start oscillation current calculation. 26) The start oscillation current curves for the operating mode and its neighboring competing modes are shown in Fig. 1.…”
Section: Mode Selection and Cold Cavity Analysismentioning
confidence: 99%
“…¼ =T (T is the transient time of the electrons through the resonator) are considered in the start oscillation current calculation. 26) The start oscillation current curves for the operating mode and its neighboring competing modes are shown in Fig. 1.…”
Section: Mode Selection and Cold Cavity Analysismentioning
confidence: 99%
“…Figure 1a and b show the SOC curves of various neighbouring modes with respect to the cavity magnetic field and the coupling coefficient as the function of the ratio of beam radius and cavity radius, respectively. The SOC is calculated for the modes lies in the amplification band Δω = π/T, where T is transient time of the electrons moving through the resonator [17]. The detuned interaction cavity magnetic field is optimized 3.8 T and thus the interaction cavity operates in the hard excitation region.…”
Section: Operating Mode Selection and Start Oscillation Current (Soc)mentioning
confidence: 99%