2001
DOI: 10.1051/epjap:2001156
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Evolution of overlimiting electron beam instability

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Cited by 12 publications
(10 citation statements)
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“…The picture described above is valid for e-beams, instability of which is due to induced radiation of the system proper waves by the beam electrons. However, it is known that with increase in beam current the physical nature of e-beam instabilities changes [6,7,[12][13][14]. This is a result of influence of the beam space charge.…”
Section: The Behavior Of Overlimiting Electron Beam Instabilitymentioning
confidence: 99%
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“…The picture described above is valid for e-beams, instability of which is due to induced radiation of the system proper waves by the beam electrons. However, it is known that with increase in beam current the physical nature of e-beam instabilities changes [6,7,[12][13][14]. This is a result of influence of the beam space charge.…”
Section: The Behavior Of Overlimiting Electron Beam Instabilitymentioning
confidence: 99%
“…Our steps coincide to those for the case of underlimiting e-beams: expand the DR (27) in series near ω 0 and k 0 (see (29) and derive an equation for SVA. Making use the condition of OB 2β 2 γ 2 δ=k 0 u ≥ 1 [13], one can obtain [6,12].…”
Section: Equation For Sva and Its Solution: Transition To The New Typmentioning
confidence: 99%
“…Detail analysis of the waveform, induced by overlimiting electron beam owing to instability development in the absence of dissipation has been done in [6]. Briefly this analysis may be reduced to following.…”
Section: Analysis Of Induced Waveformmentioning
confidence: 99%
“…to the maximal growth rate for overlimiting beam [6]. In other words the maximal growth rate of instability usually describing instability in given system in fact is nothing else that the growth rate in the peak of wave packet As the beam current increases the peak of induced waveform shifts (from 1/3of its length) backward to the middle of wave packet and the growth rate essentially changes its value and dependence on beam density [6] In a fixed point z the field E 0 (z,t) attains it's maximal value ∼ exp δ ovl z/(uv 0 ) 1/2 at the instant t = z/w a , where…”
Section: Analysis Of Induced Waveformmentioning
confidence: 99%
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