1996
DOI: 10.1109/27.532945
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Theory of gyro-backward wave oscillators with tapered magnetic field and waveguide cross section

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Cited by 61 publications
(14 citation statements)
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“…Following experiments with moderate energy electron beam and high energy electron beam were performed to obtain kilowatt-level 2,8-10 to megawatt-level [11][12][13] millimeter wave sources, but the fast tuning bandwidth was less than expected. Theoretical and simulation works were then motivated by experiments for studying the essential properties of gyro-BWO, e.g., the start oscillation criteria (linear properties), [14][15][16] the saturation efficiency of the beamwave interaction, [17][18][19][20][21][22][23] and the nonstationary oscillation of the gyro-BWO (nonlinear properties). 24,25 The theoretical analysis and numerical simulation formed the basis of the experimental design and have been extensively applied on the study of the efficiency enhancement of gyro-BWO induced by the magnetic field tapering 18,19,21 or the tapering of waveguide wall radius.…”
Section: Introductionmentioning
confidence: 99%
“…Following experiments with moderate energy electron beam and high energy electron beam were performed to obtain kilowatt-level 2,8-10 to megawatt-level [11][12][13] millimeter wave sources, but the fast tuning bandwidth was less than expected. Theoretical and simulation works were then motivated by experiments for studying the essential properties of gyro-BWO, e.g., the start oscillation criteria (linear properties), [14][15][16] the saturation efficiency of the beamwave interaction, [17][18][19][20][21][22][23] and the nonstationary oscillation of the gyro-BWO (nonlinear properties). 24,25 The theoretical analysis and numerical simulation formed the basis of the experimental design and have been extensively applied on the study of the efficiency enhancement of gyro-BWO induced by the magnetic field tapering 18,19,21 or the tapering of waveguide wall radius.…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, a gyro-device operating with a traveling-wave and a nonresonant-microwave structure can provide a broadband smooth frequency tuning by variation of the magnetic field or the electron beam energy. The gyro-BWO operation has been theoretically analyzed in detail (see, e.g., [1]- [4]) and successfully realized in a number of experiments [5]- [7]. In the experimental studies at the Naval Research Laboratory [5] and the National Tsing Hua University [6], pulsed Ka-band gyro-BWO operation at the fundamental cyclotron harmonic and fundamental mode of a smooth cylindrical waveguide was demonstrated with voltage-and magnetic-frequency tuning of up to 5% and 13%, respectively, a very high efficiency (for BWO) of nearly 20% and a pulsed power up to 100 kW.…”
Section: Introductionmentioning
confidence: 99%
“…12,13 Either cylindrical or rectangular waveguides are usually used as the interaction structures of gyro-BWOs. [1][2][3][4][5][6][7][8][9][10][11][12][13] Various transverse waveguide modes may be resonantly excited by matching the beam-wave resonance condition when the beam current exceeds their start-oscillation currents.…”
Section: Introductionmentioning
confidence: 99%
“…1 Start oscillation conditions were analyzed using the linear theory. [2][3][4] Nonlinear analysis revealed that properly tapering the magnetic field can enhance the efficiency of the gyro-BWO from 10-15% to 25-30%.…”
Section: Introductionmentioning
confidence: 99%