1996
DOI: 10.1109/16.502139
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Design of an efficient, low voltage, third harmonic, large-orbit gyrotron amplifier with a vane-resonator output cavity

Abstract: We present the design of a 100 kW, J-band, third harmonic large-orbit gyrotron amplifier which utilizes the interaction between a 45 kV, 4 A beam and a vane resonator output cavity operating in the "?r"-mode. An efficiency of 55% is predicted with a large signal gain near 20 dB by a single particle code which takes into account nonideal effects associated with finite beam thickness and finite magnetic field transition widths. High efficiency is achieved by velocity modulation of an axially-streaming annular be… Show more

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Cited by 7 publications
(2 citation statements)
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“…However, can decrease with decreasing at sufficiently small q and . As an example, this occurs for the cavities with2 Dissipative rarefaction of the complex natural frequency spectrum for the modes corresponding to the first resonance, r0 s 0.1, r s 1.75, N s 16 1 25 and the same other parameters as in Figure 1, 2 1…”
mentioning
confidence: 93%
“…However, can decrease with decreasing at sufficiently small q and . As an example, this occurs for the cavities with2 Dissipative rarefaction of the complex natural frequency spectrum for the modes corresponding to the first resonance, r0 s 0.1, r s 1.75, N s 16 1 25 and the same other parameters as in Figure 1, 2 1…”
mentioning
confidence: 93%
“…If the device can operate on a higher cyclotron harmonic number s, then the requisite magnetic field will decrease approximately by a factor of s. As the required frequencies increase, high harmonic operation is an inevitable choice. [2][3][4][5][6] High harmonic interaction is prone to mode selection problems due to the mode competition from the first and lower harmonic interactions. Fortunately, the aforementioned problems can be alleviated to a great extent by using largeorbit ͑axis-encircling͒ electron beams.…”
Section: Introductionmentioning
confidence: 99%