2005
DOI: 10.1063/1.2126815
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Dynamic of ion density perturbations observed in a microwave-plasma interaction

Abstract: The dynamical behavior of ion density perturbations propagated at low-frequency wave nature is experimentally observed in microwave-plasma interaction. An unmagnetized, inhomogeneous laboratory plasma irradiated by an obliquely incident microwave with maximum power P = 10 kW and pulse width approximately ion plasma period ͑ pi Ϸ 2 / pi ͒ is studied. The p-polarized electric-field component of the interacted microwave of frequency 0 leads to a nonlinear phenomenon driven by the ponderomotive force by the proces… Show more

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Cited by 17 publications
(6 citation statements)
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“…The plasma density modulation up to 40% was obtained when the microwave pulse duration is near the ion oscillation period. Other experimental studies of plasma wakefield generation, ponderomotive force effects, and self-focusing of microwaves (with frequencies in the range of 3-10 GHz) in plasma were also carried out [16][17][18]. All these experiments were characterized by a relatively low power microwave sources (10-250 kW) with much longer pulses (60 ns-1 µs) than the periods of the plasma electron and ion oscillation.…”
Section: Introductionmentioning
confidence: 99%
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“…The plasma density modulation up to 40% was obtained when the microwave pulse duration is near the ion oscillation period. Other experimental studies of plasma wakefield generation, ponderomotive force effects, and self-focusing of microwaves (with frequencies in the range of 3-10 GHz) in plasma were also carried out [16][17][18]. All these experiments were characterized by a relatively low power microwave sources (10-250 kW) with much longer pulses (60 ns-1 µs) than the periods of the plasma electron and ion oscillation.…”
Section: Introductionmentioning
confidence: 99%
“…The density modulation period is of the order of 1 ns over a range of~10 cm, a parameter range much more tractable than the laser/plasma experiments though realized with much lower ponderomotive forces. Early studies of the interaction of microwaves with plasmas were performed at much lower powers (<250 kW and pulse lengths of 50 ns-3 µs) [11,[15][16][17][18].…”
Section: Introductionmentioning
confidence: 99%
“…[1][2][3][4][5][6][7][8][9] In addition to these non-linear phenomena, the relativistic ponderomotive force and the relativistic mass reveal in the interaction between intense MW and plasma. A number of non-linear phenomena appear during this interaction, including resonance absorption, frequency upshift, charged particle acceleration, and high-energy super-thermal electron generation.…”
Section: Introductionmentioning
confidence: 99%
“…A number of non-linear phenomena appear during this interaction, including resonance absorption, frequency upshift, charged particle acceleration, and high-energy super-thermal electron generation. [1][2][3][4][5][6][7][8][9] In addition to these non-linear phenomena, the relativistic ponderomotive force and the relativistic mass reveal in the interaction between intense MW and plasma. These two non-linear effects arise when the intensity of the MW beam is sufficiently high.…”
Section: Introductionmentioning
confidence: 99%
“…In earlier studies, the generation of plasma waves using microwaves was experimentally investigated with relatively low microwave power ð3 À 250 kWÞ and long ð0:05 À 3 lsÞ duration pulses. [10][11][12][13] In these studies, the effects of the microwave absorption, plasma density perturbation, microwave guiding, and ponderomotive force were investigated in both over-and under-dense plasmas. Also, in Ref.…”
Section: Introductionmentioning
confidence: 99%