2009
DOI: 10.1063/1.3250928
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Onset and saturation of backward stimulated Raman scattering of laser in trapping regime in three spatial dimensions

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Cited by 57 publications
(68 citation statements)
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References 36 publications
(55 reference statements)
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“…In actual plasma, the SRS daughter LW is subject to other instabilities as well, such as LW-ion-acoustic decay (LDI). Fluid and kinetic regime LDI have been observed in SRS simulations [19,22] while kinetic regime LDI has been experimentally [23] noted [12].…”
Section: Introductionmentioning
confidence: 99%
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“…In actual plasma, the SRS daughter LW is subject to other instabilities as well, such as LW-ion-acoustic decay (LDI). Fluid and kinetic regime LDI have been observed in SRS simulations [19,22] while kinetic regime LDI has been experimentally [23] noted [12].…”
Section: Introductionmentioning
confidence: 99%
“…If a timedependent Vlasov equation solution has a symmetry, e.g., in 2 + 2D (two space and two velocity dimensions) when the initial condition (and possible external potential) only depend on one spatial coordinate z, or in 3 + 3D a cylindrically symmetric configuration, then an instability may break that symmetry, allowing for a determination of growth rate. The former, revisited here, was explored in 2 + 2D Vlasov simulations [17], while the latter was observed [19] in 3D PIC, SRS single speckle simulations. In addition, we present LW filamentation growth rates of linear fluctuations about a particular class of BGK modes, recalled in the next Section III A.…”
Section: Bgk Mode Linear Filamentation Instabilitymentioning
confidence: 99%
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“…State-of-the-art PIC codes move up to 10 11 macroparticles during ϳ10 5 time steps. 94 As sketched in Fig. 3, the PIC technique consists in representing the plasma as a collection of N macroparticles subjected to self-consistent electromagnetic fields.…”
Section: Principle Of Particle-in-cell Simulationsmentioning
confidence: 99%