2014
DOI: 10.1016/j.nima.2013.05.090
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Effects of beam-plasma instabilities on neutralized propagation of intense ion beams in background plasma

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Cited by 12 publications
(23 citation statements)
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References 9 publications
(13 reference statements)
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“…Therefore, in the case of an ion beam propagating in background plasma in the presence of the two-stream instability both the radial electric field and the reversal of the selfmagnetic field act together to defocus the beam as it propagates. Furthermore, high intensity longitudinal electric fields of plasma waves generated by two-stream instability can strongly modulate the density of propagating ion beam longitudinally -produce bunching of initially long beam pulses [34,35,36,37].…”
Section: This Paper Reviews Past Theoretical and Experimental Studies...mentioning
confidence: 99%
“…Therefore, in the case of an ion beam propagating in background plasma in the presence of the two-stream instability both the radial electric field and the reversal of the selfmagnetic field act together to defocus the beam as it propagates. Furthermore, high intensity longitudinal electric fields of plasma waves generated by two-stream instability can strongly modulate the density of propagating ion beam longitudinally -produce bunching of initially long beam pulses [34,35,36,37].…”
Section: This Paper Reviews Past Theoretical and Experimental Studies...mentioning
confidence: 99%
“…26 Note also that the neutralization of the beam charge occurs on the plasma period scale, which is less than one nanosecond for these beam parameters. In general, the fast variations of the beam density on the scales faster than the plasma period-a nanoseconds duration for our parameters may drive large amplitude plasma waves, see, e.g., Ref.…”
mentioning
confidence: 91%
“…It has been long known that the two-stream instability can strongly affect the return current formation in plasmas. [26][27][28][29][30][31][32][33][34] Under some conditions, the two-stream instability causes plasma electrons to follow the ion beam with the mean velocity approaching the beam velocity. Without the instability electrons in return current of an ion beam propagating in plasma would flow in the direction of the beam velocity with the velocity proportional to the beam velocity times ratio of the beam density to background plasma density, v b n b =n p ; this flow originates from the inductive electric field induced by the beam pulse in plasma and is formed in response to timedependent beam self-magnetic field.…”
mentioning
confidence: 99%
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