1986
DOI: 10.1080/00207218608920927
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Theory of non-stationary processes in gyrotrons with low Q resonators

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Cited by 175 publications
(81 citation statements)
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“…In this paper, we present the first detailed and systematic experimental characterization of different operating regimes, from linear to chaotic over a wide range of system parameters which will be summarized in the normalized ðD À IÞ plane with D and I being the normalized detuning and current, 9 respectively. After the seminal work by Ginzburg et al, 15 Airila et al 2 used a numerical approach to study non linear effects in gyro devices and presented their findings in the ðD À IÞ plane. The comparison with our results confirms the different nonstationary regimes analysed in Ref.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…In this paper, we present the first detailed and systematic experimental characterization of different operating regimes, from linear to chaotic over a wide range of system parameters which will be summarized in the normalized ðD À IÞ plane with D and I being the normalized detuning and current, 9 respectively. After the seminal work by Ginzburg et al, 15 Airila et al 2 used a numerical approach to study non linear effects in gyro devices and presented their findings in the ðD À IÞ plane. The comparison with our results confirms the different nonstationary regimes analysed in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…These theoretical studies were made on advanced models based on the slow-time scale formulation of the selfconsistent interaction equations 1,2,7,8,15,27 or on more firstprinciple set of equations solved using a particle in cell approach. 16,17,22 Experimental studies have been carried out by Chang et al 10 and more recently on a system where delayed feedback mechanisms were introduced for accessing to chaotic regimes.…”
Section: Introductionmentioning
confidence: 99%
“…Будем считать, что на входе в простран-ство взаимодействия электроны равномерно распределены по фазам циклотронного вращения p(Z = 0) = e iθ 0 , θ 0 ∈ [0, 2π]. При этом во входном и выходном сечениях волновода использовались излучательные граничные условия [10].…”
Section: поступило в редакцию 18 мая 2017 гunclassified
“…where the most normalized variables are the same as in the previous gyrotron model [3], At the system input and output we apply the well-known reflectionless boundary condition [3]. In Fig.…”
Section: Mechanism Of Rogue Waves Generationmentioning
confidence: 99%
“…For theoretical analysis of rogue waves generation in gyrotrons we have generalized the self-consistent timedomain model of low-Q gyrotrons [3] in the frame of which the evolution of the field amplitude is described by a non-uniform parabolic equation. In the novel model, first of all an inclination of the beam line with respect to the dispersion characteristic of the waveguide mode is taken into account [4], because the maximum spectrum bandwidth of chaotic generation, including rogue waves, is determined by the difference between resonances with backward and forward waves (points 1 and 2 in Fig.…”
Section: Mechanism Of Rogue Waves Generationmentioning
confidence: 99%